Golf club set and golf club shaft set

Abstract

Disclosed is a golf club set having harmonized golf club performance among the club numbers. In the golf club set, for at least three golf clubs, a ratio or a sum of a frequency, the frequency being measured by vibrating a tip portion of a golf club shaft constituting each of the golf clubs, and a frequency, the frequency being measured by vibrating a rear end portion of the golf club shaft, is determined in relation with order of the club number.

Description

This is a division of application Ser. No. 10/135,822, filed May 1, 2002, now U.S. Pat. No. 6,916,251, issued Jul. 12, 2005, which is hereby incorporated herein by reference. Applicants claim the benefits of 35 U.S.C. §§ 120 and 121.

BACKGROUND OF THE INVENTION

The present invention relates to a golf club set comprising a plurality of golf clubs having various different loft angles and a golf club shaft set used for the golf club set.

An iron golf club set is constituted of about 10 golf clubs from long irons to short irons, where club length and a loft angle differ for each club number so that different flying distance can be obtained for each club number.

In the foregoing golf club set, it is preferable to establish harmony on height of trajectory of a hit ball by a golf club among the club numbers. As a yardstick to evaluate the height of trajectory of a hit ball by a golf club, a kick point and the like are generally used. However, since the kick point only indicates the top position of bending of a golf club shaft, it has been difficult to show the height of trajectory of a hit ball by a golf club exactly with the yardstick. Therefore, even when a golf club set is designed to establish harmony on the height of trajectory of a hit ball by a golf club among the club numbers based on conventional yardstick, it is the present situation that harmony on actual height of trajectory of a hit ball by a golf club is not established among the club numbers.

In addition, in the foregoing golf club set, it is preferable to establish harmony on flexibility of a golf club shaft actually felt by a person among the club numbers. As a yardstick to evaluate flexibility of a golf club shaft, frequency (cpm) and the like are generally used. However, when flexibility of a golf club shaft is evaluated based on such a yardstick and even when the value is large, a person did not always actually feel stiff. Specifically, depending on the difference of a kick point, the result based on the foregoing yardstick is sometimes different. For example, in two golf club shafts having kick points different from each other, reversal phenomena that one golf club shaft indicates higher frequency than the other golf club shaft while the latter one is felt stiffer than the former one, is occurred. Therefore, even when a golf club set is designed to establish harmony on flexibility of a golf club shaft based on conventional yardstick among the club numbers, it is the present situation that harmony on flexibility of golf club shafts actually felt by a person is not obtained among the club numbers.

SUMMARY OF THE INVENTION

The first object of the present invention is to provide a golf club set and a golf club shaft set wherein height of trajectory of a hit ball by a golf club is harmonized among the club numbers.

The second object of the present invention is to provide a golf club set and a golf club shaft set wherein flexibility of a golf club shaft actually felt by a person is harmonized among the club numbers.

A golf club set to achieve the foregoing first object in accordance with the present invention comprises a plurality of golf clubs in which a golf club head is assembled on a tip portion of a golf club shaft, the plurality of golf clubs having loft angles different in each club number, wherein, in at least three golf clubs among the plurality of golf clubs, a ratio of a frequency, the frequency being measured by vibrating a tip portion of a golf club shaft constituting each of the golf clubs in a state that a rear end portion of the golf club shaft is fastened, and a frequency, the frequency being measured by vibrating the rear end portion of the golf club shaft in a state that the tip portion of the golf club shaft is fastened, is determined in relation with order of the club number. The ratio of frequencies is preferably varied almost linearly in accordance with order of the club number.

When the foregoing ratio of frequencies is varied almost linearly in accordance with order of the club number, it is preferable to satisfy the following conditions in the present invention.

Specifically, in a golf club set comprising a plurality of golf clubs in which a golf club head is assembled on a tip portion of a golf club shaft, the plurality of golf clubs having loft angles different in each club number, the plurality of golf clubs include a group of at least three golf clubs having loft angles in a range of 16 degree or more and 41 degree or less. Further, all of the golf clubs in the group are denoted by continuous natural numbers X starting at 1 in order of increasing loft angle from the lowest loft angle. In addition, a ratio of frequencies calculated from a frequency as a numerator, the frequency being measured by vibrating a tip portion of a golf club shaft constituting each of the golf clubs in a state that a rear end portion of the golf club shaft is fastened, and a frequency as a denominator, the frequency being measured by vibrating the rear end portion of the golf club shaft in a state that the tip portion of the golf club shaft is fastened, is denoted by Z.

In this case, the ratio Z of frequencies is determined so that an estimated error to a regression line is 0.05 or less, when a distribution of the ratio Z of frequencies to the natural number X in all of the golf clubs in the group is fitted on the regression line.

More preferably, when a sum of the frequency which is measured in the state that the rear end portion of the golf club shaft is fastened and the frequency which is measured in the state that the tip portion of the golf club shaft is fastened is denoted by Y (cpm), the sum Y of frequencies is determined so that an estimated error to a regression line is 30 cpm or less, when a distribution of the sum Y of frequencies to the natural number X in all of the golf clubs in the group is fitted on the regression line.

Another golf club set to achieve the foregoing first object in accordance with the present invention comprises a plurality of golf clubs in which a golf club head is assembled on a tip portion of a golf club shaft, the plurality of golf clubs having loft angles different in each club number, wherein, in at least three golf clubs among the plurality of golf clubs, a ratio of a frequency, the frequency being measured by vibrating a tip portion of a golf club shaft constituting each of the golf clubs in a state that a rear end portion of the golf club shaft is fastened, and a frequency, the frequency being measured by vibrating the rear end portion of the golf club shaft in a state that the tip portion of the golf club shaft is fastened, is determined in relation with order of size of the loft angle. The ratio of frequencies is preferably varied corresponding to order of size of the loft angle almost linearly.

When the foregoing ratio of frequencies is varied almost linearly in accordance with order of size of the loft angle, it is preferable to satisfy the following conditions in the present invention.

Specifically, in a golf club set comprising a plurality of golf clubs in which a golf club head is assembled on a tip portion of a golf club shaft, the plurality of golf clubs having loft angles different in each club number, the plurality of golf clubs include a group of at least three golf clubs having loft angles in a range of 16 degree or more and 41 degree or less. Further, the loft angles of the golf clubs in the group are denoted by θ (degree). In addition, a ratio of frequencies calculated from a frequency as a numerator, the frequency being measured by vibrating a tip portion of a golf club shaft constituting each of the golf clubs in a state that a rear end portion of the golf club shaft is fastened, and a frequency as a denominator, the frequency being measured by vibrating the rear end portion of the golf club shaft in a state that the tip portion of the golf club shaft is fastened, is denoted by Z.

Then, the ratio Z of frequencies is determined so that an estimated error to a regression line is 0.05 or less, when a distribution of the ratio Z of frequencies to the loft angle θ in all of the golf clubs in the group is fitted on the regression line.

More preferably, when a sum of the frequency which is measured in the state that the rear end portion of the golf club shaft is fastened and the frequency which is measured in the state that the tip portion of the golf club shaft is fastened, is denoted by Y (cpm), the sum Y of frequencies is determined so that an estimated error to a regression line is 30 cpm or less, when a distribution of the sum Y of frequencies to the loft angle θ in all of the golf clubs in the group is fitted on the regression line.

In the present invention, a ratio of a frequency, the frequency being measured by vibrating a tip portion of a golf club shaft in a state that a rear end portion of the golf club shaft is fastened, and a frequency, the frequency being measured by vibrating the rear end portion of the golf club shaft in a state that the tip portion of the golf club shaft is fastened, is used as a yardstick for height of trajectory of a hit ball by the golf club. Since the ratio of frequencies is composed of a combination of frequency performance obtained in a state that a rear end portion of a golf club shaft is fastened and frequency performance obtained in a state that a tip portion of the golf club shaft is fastened, it indicates bending characteristics of a golf club shaft well, and it also indicates height of trajectory of a hit ball by a golf club more exactly with numeral values. Therefore, when the ratio of frequencies has a correlation with order of the club number or order of loft angle size, a sense of incongruity such that in only specified golf clubs through a golf club set, a trajectory in accordance with a loft angle can not be obtained, can be avoided.

Measurement of frequency is preferably carried out as a simple golf club shaft. It is possible to adjust golf clubs as a whole golf club set with more accuracy by measuring frequency of a simple golf club shaft, adjusting it, adjusting other parts appropriately and fabricating a golf club. Accordingly, harmonized height of trajectory of a hit ball through a whole golf club set is obtained more exactly.

The club number is mainly identification information on an order of loft angle denoted by numbers, letters, marks and the like, which are added on golf clubs, so that golf clubs having different loft angles can be placed in order of loft angle and a loft angle of each club number is decided with a constant difference or almost constant difference appropriately among those skilled in the art. Moreover, a bigger club number means a club number for a bigger loft angle.

The present invention also includes golf club shaft sets before those are fabricated as golf club. A golf club shaft set is generally composed of a plurality of golf club shafts having different length, and those golf club shafts in order of longer shaft length are assembled in golf club heads in order of smaller loft angle to become golf clubs. Those skilled in the art may use the golf club shafts in the golf club shaft set as they are or may use after cutting if necessary when they fabricate golf clubs.

A golf club shaft set to achieve the foregoing first object in accordance with the present invention comprises a plurality of golf club shafts to constitute a golf club set, wherein, in at least three golf club shafts among the plurality of golf club shafts, a ratio of a frequency, the frequency being measured by vibrating a tip portion of a golf club shaft in a state that a rear end portion of the golf club shaft is fastened, and a frequency, the frequency being measured by vibrating a rear end portion of the golf club shaft in a state that a tip portion of the golf club shaft is fastened, is determined in relation with order of the club number and preferably it is varied almost linearly in accordance with order of the club number.

When the foregoing ratio of frequencies is varied almost linearly in accordance with order of the club number, it is preferable to satisfy the following conditions in the present invention.

Specifically, in a golf club shaft set comprising a plurality of golf club shafts to constitute a golf club set, the plurality of golf club shafts must include a group of at least three golf club shafts. The group of golf club shafts is preferably composed of golf club shafts, which are combined to golf clubs having loft angles in a range of 16 degree or more and 41 degree or less. Further, all of the golf club shafts in the group are denoted by continuous natural numbers X starting at 1 in order from the largest golf club shaft length. In addition, a ratio of frequencies calculated from a frequency as a numerator, the frequency being measured by vibrating a tip portion of a golf club shaft in a state that a rear end portion of the golf club shaft is fastened, and a frequency as a denominator, the frequency being measured by vibrating a rear end portion of the golf club shaft in a state that a tip portion of the golf club shaft is fastened, is denoted by Z.

Then, when a distribution of the foregoing ratio Z of frequencies is fitted on a regression line to the foregoing natural number X in all of the golf club shafts of the foregoing group, the foregoing ratio Z of frequencies is set so that estimated error to the regression line is 0.05 or less.

More preferably, when the sum of a frequency measured in the state that a rear portion of the golf club shaft is fastened and a frequency measured in the state that a tip portion of the golf club shaft is fastened is denoted by Y (cpm). Then, when a distribution of the foregoing sum Y of frequencies is fitted on a regression line to the foregoing natural number X for all of the foregoing golf club shafts, the foregoing sum Y of frequencies is set so that an estimated error to the regression line is 30 cpm or less.

Other golf club shaft set to achieve the foregoing first object in accordance with the present invention comprises a plurality of golf club shafts to constitute a golf club set, wherein in at least three golf club shafts among the plurality of golf club shafts, a ratio of a frequency, the frequency being measured by vibrating a tip portion of a golf club shaft in a state that a rear end portion of each golf club shaft is fastened, and a frequency, the frequency being measured by vibrating a rear end portion of the golf club shaft in a state that a tip portion of the golf club shaft is fastened, is determined in relation with order of golf club shaft length and preferably it is varied almost linearly corresponding to golf club shaft length.

When the foregoing ratio of frequencies is varied almost linearly corresponding to order of length of the golf club shaft, it is preferable to satisfy the following conditions in the present invention.

Specifically, in a golf club shaft set comprising a plurality of golf club shafts to constitute a golf club set, the foregoing golf club shafts include a group of at least three golf club shafts. The group of golf club shafts is preferably composed of golf club shafts, which are assembled to golf clubs having loft angles in a range of 16 degree or more and 41 degree or less. The length of the golf club shaft is denoted by L (mm), and, in addition, a ratio of frequencies calculated from a frequency as a numerator, the frequency being measured by vibrating a tip portion of a golf club shaft in a state that a rear end portion of each golf club shaft is fastened, and a frequency as a denominator, the frequency being measured by vibrating a rear end portion of the golf club shaft in a state that a tip portion of the golf club shaft is fastened, is denoted by Z.

Then, when a distribution of the foregoing ratio Z of frequencies to the foregoing length L is fitted on a regression line in all of the golf club shafts of the foregoing group, the foregoing ratio Z of frequencies is set so that estimated error to the regression line is 0.05 or less.

More preferably, when the sum of a frequency which is measured in the state that a rear portion of the foregoing golf club shaft is fastened and a frequency which is measured in the state that a tip portion of the golf club shaft is fastened, is denoted by Y (cpm) and when a distribution of the foregoing sum Y of frequencies to the foregoing length is fitted on a regression line L, the foregoing sum Y of frequencies is set so that estimated error to the regression line is 30 cpm or less.

As described above, in a golf club shaft set, when the ratio of frequencies has a correlation with order of the club number or order of length of golf club shafts, a sense of incongruity such that in only specified golf clubs through a golf club set, a trajectory in accordance with a loft angle can not be obtained, can be avoided.

On the other hand, a golf club set to achieve the foregoing second object in accordance with the present invention comprises a plurality of golf clubs in which a golf club head is assembled on a tip portion of a golf club shaft, wherein the plurality of golf clubs have different loft angles in each club number, wherein, in at least three golf clubs among the plurality of golf clubs, a sum of a frequency, the frequency being measured by vibrating a tip portion of a golf club shaft constituting each of the golf clubs in a state that a rear end portion of the golf club shaft is fastened, and a frequency, the frequency being measured by vibrating the rear end portion of the golf club shaft in a state that the tip portion of the golf club shaft is fastened, is determined in relation with order of the club number and preferably it is varied almost linearly corresponding to order of the club number.

When the foregoing ratio of frequencies is varied almost linearly corresponding to order of the club number, it is preferable to satisfy the following conditions in the present invention.

Specifically, in a golf club set comprising a plurality of golf clubs in which a golf club head is assembled on a tip portion of a golf club shaft, loft angles of which are different in each club number, wherein the plurality of golf clubs must include a group of at least three golf clubs having loft angles in a range of 16 degree or more and 41 degree or less. All of the golf clubs in the group are denoted by continuous natural number X starting at 1 in order from the smallest loft angle, and, in addition, the sum of a frequency, the frequency being measured by vibrating a tip portion of a golf club shaft in a state that a rear end portion of the golf club shaft is fastened for a length of 178 mm from the rear end and a 200 g weight is loaded on a tip portion for a length of 30 mm from the tip end, and a frequency, the frequency being measured by vibrating the rear end portion of the golf club shaft in a state that the tip portion of the golf club shaft is fastened for a length of 178 mm from the tip end and a 200 g weight is loaded on the rear end portion for a length of 30 mm from the rear end, is denoted by Y (cpm).

Then the foregoing sum Y of frequencies is determined in a range of the following formula (1) to the foregoing natural number X in all of the golf clubs of the foregoing group,
aX+b≦Y≦aX+b+12  (1)
where coefficients a and b are arbitrary constants.

Alternatively, when a distribution of the foregoing sum Y of frequencies to the foregoing natural number X is fitted on a regression line, the foregoing sum Y of frequencies is determined so that estimated error to the regression line is 8 (cpm) or less in all of the golf clubs in the foregoing group.

More preferably, when a ratio of frequencies calculated from a frequency as a numerator, the frequency being measured in the state that the rear end portion of the golf club shaft is fastened, and a frequency as a denominator, the frequency being measured in the state that the tip portion of the golf club shaft is fastened, is denoted by Z, the ratio Z of frequencies is determined so that an estimated error to a regression line is 0.15 or less, when a distribution of the ratio Z of frequencies to the natural number X in all of the golf clubs in the group is fitted on the regression line.

Another golf club set to achieve the foregoing second object in accordance with the present invention comprises a plurality of golf clubs in which a golf club head is assembled on a tip portion of a golf club shaft, the plurality of golf clubs having loft angles different in each club number, wherein, in at least three golf clubs among the plurality of golf clubs, a sum of a frequency, the frequency being measured by vibrating a tip portion of a golf club shaft constituting each of the golf clubs in a state that a rear end portion of the golf club shaft is fastened, and a frequency, the frequency being measured by vibrating the rear end portion of the golf club shaft in a state that the tip portion of the golf club shaft is fastened, is determined in relation with order of size of the loft angle. The sum of frequencies is preferably varied corresponding to order of size of the loft angle almost linearly.

When the foregoing sum of frequencies is varied almost linearly corresponding to order of size of the loft angle, it is preferable to satisfy the following conditions in the present invention.

Specifically, in a golf club set comprising a plurality of golf clubs in which a golf club head is assembled on a tip portion of a golf club shaft, the plurality of golf clubs having loft angles different in each club number, the plurality of golf clubs include a group of at least three golf clubs having loft angles in a range of 16 degree or more and 41 degree or less. Further, the loft angles in the group are denoted by 0 (degree). In addition, a sum of a frequency, the frequency being measured by vibrating a tip portion of a golf club shaft to constituting each of the golf clubs in a state that a rear end portion of the golf club shaft is fastened for a length of 178 mm from the rear end and a 200 g weight is loaded on the tip portion for a length of 30 mm from the tip end, and a frequency, the frequency being measured by vibrating the rear end portion of the golf club shaft in a state that the tip portion of the golf club shaft is fastened for a length of 178 mm from the tip end and a 200 g weight is loaded on the rear end portion for a length of 30 mm from the rear end, is denoted by Y (cpm).

Then, the sum Y of frequencies is determined in a range of the following formula (2) to the loft angle θ in all of the golf clubs of the group,
cθ+d≦Y≦cθ+d+12  (2)
where coefficients c and d are arbitrary constants.

Alternatively, for all of the golf clubs in the foregoing group, the foregoing sum Y of frequencies is determined so that an estimated error to a regression line is 8 (cpm) or less, when a distribution of the foregoing sum Y of frequencies to the foregoing loft angle θ is fitted on the regression line.

More preferably, when a ratio of frequencies calculated from a frequency as a numerator, the frequency being measured in the state that the rear end portion of the golf club shaft is fastened, and a frequency as a denominator, the frequency being measured in the state that the tip portion of the golf club shaft is fastened, is denoted by Z, the ratio Z of frequencies is determined so that an estimated error to a regression line is 0.15 or less, when a distribution of the ratio Z of frequencies to the loft angle θ in all of the golf clubs in the group is fitted on the regression line.

In the present invention, a sum of a frequency, the frequency being measured by vibrating a tip portion of a golf club shaft in a state that a rear end portion of a golf club shaft is fastened, and a frequency, the frequency being measured by vibrating the rear end portion of the golf club shafts in a state that the tip portion of the golf club shafts is fastened, is used as a yardstick for flexibility of a golf shaft. Since the sum of frequencies is composed of a combination of frequency performance obtained in a state that a rear end portion of a golf club shaft is fastened and frequency performance obtained in a state that a tip portion of the golf club shaft is fastened, it indicates flexibility of a golf club shaft more exactly with numeral values regardless of location of kick point. Therefore, when the sum of frequencies has a correlation with order of the club number or order of loft angle size, a sense of incongruity such that only specified golf clubs through a golf club set are felt stiffer, can be avoided.

Measurement of frequency is preferably carried out as a simple golf club shaft. It is possible to adjust golf clubs as a whole golf club set with more accuracy by measuring a frequency of a simple golf club shaft, adjusting it, adjusting other parts appropriately and fabricating a golf club. Accordingly, it is possible to harmonize flexibility actually felt by a person among the club numbers.

The club number is mainly identification information on an order of loft angles denoted on each golf club by numbers, letters, marks and the like so that golf clubs having different loft angle can be placed in order of loft angles, and a loft angle for each club number is decided with a constant difference or almost constant difference appropriately among ones skilled in the art. Further, a bigger club number means a club number having a bigger loft angle.

The present invention also includes golf club shaft sets before those are fabricated as golf club sets. A golf club shaft set is generally composed of a plurality of golf shafts having different length, and those golf shafts in order of decreasing shaft length are assembled in golf club heads in order of increasing loft angle to become golf clubs. Ones skilled in the art may use the golf club shafts of the golf club shaft set as they are or may use after cutting if necessary when they fabricate golf clubs.

A golf club shaft set to achieve the foregoing second object in accordance with the present invention comprises a plurality of golf club shafts to constitute a golf club set, wherein in at least three golf club shafts among the plurality of golf club shafts, a sum of a frequency, the frequency being measured by vibrating a tip portion of a golf club shaft in a state that a rear end portion of the golf club shaft is fastened, and a frequency, the frequency being measured by vibrating the rear end portion of the golf club shaft in a state that the tip portion of the golf club shaft is fastened, is determined in relation with order of the club number and preferably it is varied almost linearly corresponding to order of the club number.

When the foregoing sum of frequencies is varied almost linearly corresponding to order of the club number, it is preferable to satisfy the following conditions in the present invention.

Specifically, in a golf club shaft set comprising a plurality of golf club shafts to constitute a golf club set, the plurality of golf club shafts must include a group of at least three golf club shafts. The group of the golf club shafts is preferably composed of golf club shafts, which are assembled in golf clubs having loft angles in a range of 16 degree or more and 41 degree or less. And all of the golf club shafts of the group are denoted by continuous natural number X starting at 1 in order from the longest length of golf club shaft. In addition, a sum of a frequency, the frequency being measured by vibrating a tip portion of a golf club shaft in a state that a rear end portion of the golf club shaft is fastened for a length of 178 mm from the rear end and a 200 g weight is loaded on a tip portion for a length of 30 mm from the tip, and a frequency, the frequency being measured by vibrating the rear end portion of the golf club shaft in a state that the tip portion of the golf club shaft is fastened for a length of 178 mm from the tip and a 200 g weight is loaded on a rear end portion for a length of 30 mm from the rear end, is denoted by Y (cpm).

At this time, when a distribution of the foregoing sum Y of frequencies to the foregoing natural number X is fitted on a regression line, the foregoing sum Y of frequencies is determined so that estimated error to the regression line is 8 (cpm) or less in all of the golf club shafts in the foregoing group.

More preferably, a ratio of frequencies calculated from a frequency as a numerator, the frequency being measured in a state that a rear end portion of the foregoing golf club shafts is fastened, and a frequency as a denominator, the frequency being measured in a state that a tip portion of the golf club shafts is fastened, is denoted by Z. Then, when a distribution of the foregoing ratio Z of frequencies to the foregoing natural number X is fitted on a regression line in all of the golf club shafts of the foregoing group, the foregoing ratio Z of frequencies is determined so that estimated error to the regression line is 0.15 or less.

Moreover, other golf club shaft sets to achieve the foregoing second object in accordance with the present invention comprises a plurality of golf club shafts to constitute a golf club set, wherein, in at least three golf club shafts among the plurality of golf club shafts, a sum of a frequency, the frequency being measured by vibrating a tip portion of each of the golf club shafts in a state that a rear end portion of the golf club shaft is fastened, and a frequency, the frequency being measured by vibrating the rear end portion of the golf club shaft in a state that the tip portion of the golf club shaft is fastened, is determined in relation with an order of length of golf club shafts and preferably it is varied almost linearly corresponding to an order of length of golf club shafts.

When the foregoing sum of frequencies is varied almost linearly corresponding to order of length of golf club shafts, it is preferable to satisfy the following conditions in the present invention.

Specifically, in a golf club shaft set comprising a plurality of golf club shafts to constitute a golf club set, the plurality of golf club shafts must include a group of at least three golf club shafts. The group of the golf club shafts is preferably composed of golf club shafts, which are assembled in golf clubs having loft angles in a range of 16 degree or more and 41 degree or less. The length of the golf club shafts in the group is denoted by L (mm). In addition, the sum of a frequency, which is measured by vibrating a tip portion of a golf club shaft in a state that a rear end portion of the golf club shaft is fastened for a length of 178 mm from the rear end and a 200 g weight is loaded on a tip portion for a length of 30 mm from the tip and a frequency, which is measured by vibrating the rear end portion of the golf club shaft in a state that the tip portion of the golf club shaft is fastened for a length of 178 mm from the tip and a 200 g weight is loaded on the rear end portion for a length of 30 mm from the rear end, is denoted by Y (cpm).

At this time, when a distribution of the foregoing sum Y of frequencies to the foregoing length L is fitted on a regression line, the foregoing sum Y of frequencies is determined so that estimated error to the regression line is 8 (cpm) or less in all of the golf club shafts in the foregoing group.

More preferably, a ratio of frequencies calculated from a frequency as a numerator, the frequency being measured in a state that a rear end portion of the foregoing golf club shafts is fastened, and a frequency as a denominator, the frequency being measured in a state that the tip portion of the golf club shafts is fastened, is denoted by Z. Then, when a distribution of the foregoing ratio Z of frequencies to the foregoing length L is fitted on a regression line in all of the golf club shafts of the foregoing group, the foregoing ratio Z of frequencies is determined so that estimated error to the regression line is 0.15 or less.

As described above, if the sum of frequencies in a golf club shaft set has a correlation with order of the club number or order of length of golf club shafts, when it is constituted to a golf club set, a sense of incongruity such that only specified golf clubs through a golf club set are felt stiffer, can be avoided.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 is a side view showing a plurality of iron golf clubs to compose a golf club set in accordance with preferred embodiments in the present invention, omitting a part of them.

FIG. 2 is a side view showing a golf club head to explain a loft angle θ.

FIG. 3 is a perspective view showing a device for measuring the center of gravity of a golf club head.

FIG. 4 shows a method to measure the center of gravity of a golf club head and is a side view showing a state that a golf club head is placed on a device for measuring the center of gravity.

FIGS. 5(a) and 5(b) show a method to measure the center of gravity of a golf club head. FIG. 5(a) is a side view showing a state that a golf club head is placed on a device for measuring the center of gravity in the position to balance, and FIG. 5(b) is a side view showing a state that a golf club head is placed on a device for measuring the center of gravity in a position not to balance.

FIG. 6 shows a method to confirm a degree of horizontal level of a support of a device for measuring the center of gravity and is a side view showing a state that a level vial is placed on the device for measuring the center of gravity.

FIG. 7 is a side view of a device of measuring a frequency to explain a method to measure a frequency in a state that a rear end portion of a golf club shaft is fastened.

FIG. 8 is a side view of a device of measuring frequency to explain a method to measure a frequency in a state that a tip portion of a golf club shaft is fastened.

FIG. 9 is a perspective view showing a golf club shaft having a reference line.

FIG. 10 is a plane view showing a state that a rear portion of the golf club shaft of FIG. 9 is fastened to the device of measuring a frequency.

FIG. 11 is a plane view showing a state that a tip portion of the golf club shaft of FIG. 9 is fastened to the device of measuring a frequency.

FIG. 12 is a side view showing a state that the rear portion of the golf club shaft of FIG. 9 is fastened to the device of measuring a frequency.

FIG. 13 is a side view showing a state of the tip portion of the golf club shaft of FIG. 9 is fastened to the device of measuring a frequency.

FIG. 14 is a front view showing a golf club using the golf club shaft of FIG. 9.

FIG. 15 is a side view showing a shaft vibration direction in the device of measuring a frequency.

FIG. 16 is a side view showing a main direction of a shaft bending during swinging a golf club.

FIG. 17 is a perspective view showing a golf club shaft having a reference line and a logo mark added thereto in coaxial relation to each other.

FIG. 18 is a front view showing a golf club using the golf club shaft of FIG. 17.

FIG. 19 is a side view showing a golf club using a golf club shaft of FIG. 20 from a toe side.

FIG. 20 is a perspective view showing the golf club shaft having a reference line and a logo mark added on different positions in a circumferential direction.

FIG. 21 is a side view showing another golf club using the golf club shaft of FIG. 9 from a toe side.

FIG. 22 is a side view showing a state of a rear end portion of a golf club fastened to a device of measuring a frequency used for a conventional evaluation method of a golf club.

FIG. 23 is a front view showing a golf club having a grip attached to a rear end portion of a golf club shaft according to the present invention.

FIG. 24 is a front view showing an example of a golf club, where a tip portion of a golf club shaft is thicker than a rear end portion, according to the present invention.

FIG. 25 is a front view showing a golf club, where a portion of a golf club shaft constitutes a grip portion, according to the present invention.

FIGS. 26(a) and 26(b) are plane views, each thereof showing a portion of a golf club shaft fastened to a device of measuring a frequency.

FIG. 27 is a perspective view showing an example of a weight used in the present invention.

FIGS. 28(a) and 28(b) are respectively development and plane views, each thereof showing the weight of FIG. 27.

FIG. 29 is a graph showing relations between natural numbers X and ratios Z of frequencies according to the present invention.

FIG. 30 is a graph showing relations between loft angles θ and the ratios Z of frequencies according to the present invention.

FIG. 31 is a graph showing relations between length L of golf club shafts and ratios Z of frequencies according to the present invention.

FIG. 32 is a graph showing relations between the natural numbers X and sums Y of frequencies according to the present invention.

FIG. 33 is a graph showing relations between the loft angles θ and the sums Y of frequencies according to the present invention.

FIG. 34 is a graph showing relations between the length L of golf club shafts and the sums Y of frequencies according to the present invention.

FIG. 35 to FIG. 54 are graphs showing regression lines of the ratios Z of frequencies to the natural numbers X in golf club sets in examples 1 to 18 and comparative examples 1 to 2, respectively.

FIG. 55 to FIG. 74 are graphs showing regression lines of the ratios Z of frequencies to the loft angles θ in the golf club sets in the examples 1 to 18 and the comparative examples 1 to 2, respectively.

FIG. 75 to FIG. 94 are graphs showing regression lines of the ratios Z of frequencies to the length L of golf club shafts in the golf club sets in the examples 1 to 18 and the comparative examples 1 to 2, respectively.

FIG. 95 to FIG. 114 are graphs showing relations between the natural numbers X and the sums Y of frequencies in the golf club sets in the examples 1 to 18 and the comparative examples 1 to 2, respectively.

FIG. 115 to FIG. 134 are graphs showing relations between the loft angle θ and the sums Y of frequencies in the golf club sets in the examples 1 to 18 and the comparative examples 1 to 2, respectively.

FIG. 135 to FIG. 154 are graphs showing regression lines of the sums Y of frequencies to the natural numbers X in the golf club sets in the examples 1 to 18 and the comparative examples 1 to 2, respectively.

FIG. 155 to FIG. 174 are graphs showing regression lines of the sums Y of frequencies to the loft angles θ in the golf club sets in the examples 1 to 18 and the comparative examples 1 to 2, respectively.

FIG. 175 to FIG. 194 are graphs showing regression lines of the sums Y of frequencies to the length L of golf club shafts in the golf club sets in the examples 1 to 18 and the comparative examples 1 to 2, respectively.

DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS

Next, constituents of the present invention will be described with reference to the accompanying drawings in detail.

FIG. 1 shows an example of a golf club set according to the preferred embodiments in the present invention comprising nine pieces of golf clubs A3 to A9 (3 iron to 9 iron), a golf club PW (pitching wedge) and a golf club SW (sand wedge). Each golf club has a structure that a grip 2 is assembled in a rear end portion of a golf club shaft 1 and a golf club head 3 is assemble in a tip portion of a golf club shaft 1.

It is determined that in these golf clubs A3 to A9, PW and SW, the bigger the club number is, the bigger a loft angle θ (degree) of a face plane 4 to a shaft axis is as well as the shorter club length is. Specifically, it is determined that the bigger the club number is, the shorter flying distance of a hit ball is. For example the loft angle θ of the golf clubs A3 to A9, PW and SW are determined to be respectively 20 degree, 24 degree, 28 degree, 32 degree, 36 degree, 40 degree, 44 degree, 48 degree, and 58 degree. It means this golf club set comprises 3 pieces or more of golf clubs with loft angles θ in a range of 16 degree to 41 degree, preferably 5 pieces or more.

In the foregoing golf club set, it is necessary to establish harmony among, in particular, golf clubs having loft angles θ being in a range of 16 degree to 41 degree. The reason is that harmonized performance is required to those clubs in the range so that flying distance can be different corresponding to the club number. On the contrary, a golf club having a loft angle less than 16 degree is a golf club to be used mainly for hitting a ball on a tee and, so to speak, is a golf club to pursue long flying distance without any relation with swing patterns of other clubs. So it is not necessarily needed to establish harmony within a golf club set. On the other hand, a golf club having a loft angle more than 41 degree is mostly used for control shots or approach shots where swing force must be controlled and, so to speak, is a golf club, controllability of which is regarded to be important without any relation with swing patterns of other clubs. Therefore it is not necessarily needed to establish harmony within a golf club set.

The foregoing loft angle θ, as shown in FIG. 2, is an angle which a plane P forms with the face plane 4, when a golf club head 3 is placed on a standard plane B according to lie angle, the plane P including the shaft axis and orthogonal to the standard plane B is supposed, and the face plane 4 is turned to targeted direction orthogonal to the plane P. This loft angle θ is measured at the position of a sweet spot of the face plane 4. The sweet spot is an intersecting point g, at which a perpendicular drawn from the center of gravity G of the golf club head 3 to the face plane 4 intersects the face plane 4. Specifically, in either case that the face plane 4 is a plane or a curved surface, the loft angle θ is specified by setting the sweet spot as a contact point.

Measurement of the loft angle θ can be performed by use of measuring device such as a golf club head gauge manufactured by Sheng Feng Company (Taiwan), a golf club angle measurement apparatus manufactured by Golf Garage, a golf club gauge manufactured by Golfsmith and the like. These devices may be conventional ones and is not limited particularly in the present invention.

This measurement of the loft angle θ may be performed not only in a state of a golf club but also in a state that a shaft pin is inserted in a simple golf club head. Numerical value of the loft angle θ measured in a simple golf club head is substantially the same as a value of the loft angle θ obtained at the measurement of a golf club itself.

The intersecting point g on the face plane 4 indicating the position of the foregoing sweet spot is obtained by use of a measuring device of the center of gravity 41 as shown in FIG. 3. The measuring device of the center of gravity 41 has a supporting portion 42 to support an object to be measured at the top area and this supporting portion 42 can specify a position of the object, which may support the object in balance. Specifically, a measuring method of the center of gravity, as shown in FIG. 4, is to place a golf club head 3 on the supporting portion 42 and find a balanced position where the golf club head is not dropped even when holding by hand is released. Specifically, as shown in FIG. 5(a), when the point g is included in contact point of the face plane 4 and the supporting portion 42, the golf club head 3 placed on the supporting portion 42 is not dropped when holding by hand is released, but, as shown in FIG. 5(b), the point g is not included in contact point of the face plane 4 and the supporting portion 42, the golf club head 3 placed on the supporting portion 42 is dropped when holding by hand is released. Using this phenomenon, the point g is obtained.

The supporting portion 42 has preferably a shape of a plane support or supports by three points or more. Further, the area of the supporting portion 42 is preferably 15 mm² or less. The lowest limit is not specified as far as a golf club head 3 can be supported. The area of the supporting portion 42 is indicated in the area of plane portion when it is a plane and indicated in the area of a figure formed by connecting the points when it is a shape of supports by three points or more. The area of the supporting portion 42 is determined in the foregoing range, and the point g can be obtained more exactly.

A plane supported by the supporting portion 42 is preferably horizontal or almost horizontal. Here, almost horizontal means that gradient to horizontal plane is within 2 degree, preferably within 1 degree. Whether it is horizontal or almost horizontal, or not, can be confirmed and be adjusted by placing a plane plate 51 on the supporting portion 42 and thus supporting the plane plate, then placing a level 52 on the plane plate 51 as shown, in FIG. 6, for example. By determining the gradient within the foregoing range, the point g can be obtained more exactly.

Here, placing according to lie angle means a state that a gap between a round of a sole surface of the golf club head 3 and the standard plane is almost equal at an edge of toe side of the sole surface and an edge of heel side. When the round of the sole surface is not clear, it is determined by placing the golf club head so that score lines are parallel to the standard plane. When the parallel to the standard plane can not be judged in the case that the round of the sole surface is not clear and in addition the score lines are not straight lines and the like, it is determined by using a formula, lie angle (degree)=(100−club length (inches)). For example, when the golf club length is 36 inches, the lie angle is 100−36=64 degree.

The club length is measured in accordance with Traditional Standard Measuring Method, which is standardized by Japan Golf Goods Association. Specifically, it is length from a contact point of the sole surface and a back portion of a neck of a golf club head to a grip end (round portion of a cap is not included). As a measuring device, Club Measure II manufactured by Kamoshita Seikosho Co. is included.

In the foregoing golf club set, regarding the golf clubs having the loft angles in a range of 16 degree to 41 degree, a ratio of a frequency f1 (cpm), the frequency f1 being measured by vibrating a tip portion of a golf club shaft 1 constituting each of the golf clubs in a state that a rear end portion of the golf club shaft 1 is fastened, and a frequency f2 (cpm), the frequency f2 being measured by vibrating the rear end portion of the golf club shaft in a state that the tip portion of the golf club shaft 1 is fastened, is varied almost linearly corresponding to order of the club number or order of size of the loft angle θ.

Further, in the foregoing golf club set, regarding the golf clubs having the loft angle θ in a range of 16 degree to 41 degree, a sum of the frequency f1 (cpm), the frequency f1 being measured by vibrating a tip portion of a golf club shaft 1 constituting each of the golf clubs in a state that a rear end portion of the golf club shaft 1 is fastened, and a frequency f2 (cpm), the frequency f2 being measured by vibrating the rear end portion of the golf club shaft 1 in a state that the tip portion of the golf club shaft 1 is fastened, is varied almost linearly corresponding to order of the club number or order of size of the loft angle θ.

A method to adjust the size of the ratio of frequencies among the club numbers is not limited specifically, and, for example, a method by adjusting cutting length at the tip portion or the rear end portion of a shaft material is included. For example, when a simple shaft material having a length of 1000 mm is cut into 960 mm to fabricate the golf club shaft and the golf club is fabricated by using the golf club shaft, there is difference in the ratio of frequencies and the sum of frequencies between the case that 40 mm of the rear end portion of the shaft material is cut and the case that 40 mm of the tip portion of the shaft material is cut. By using this fact, it is possible to adjust the sizes of the ratio and the sum of frequencies among the club numbers. Of course at the stage of designing golf club shafts, the sizes of the ratio and the sum of frequencies may be adjusted by determining flexural rigidity and the like among the club numbers.

Next, a method to measure a frequency of a golf club shaft is described. The frequency is measured by use of a device of measuring a frequency 10 as shown in FIG. 7 and FIG. 8. The device of measuring a frequency 10 comprises a chuck 11 to fasten one of the ends of a golf club shaft 1 of the golf club and a measuring portion 12 where a frequency of the other end of a golf club shaft 1 is measured by use of a photo sensor. Such a device of measuring frequencies may be conventional one available in the market, for example, Club Timing Harmonizer (manufactured by Fujikura Rubber Industry Co.) and the like are exemplified.

Using the foregoing device 10 of measuring frequencies, as shown in FIG. 7, the rear end of a golf club shaft 1 is fastened to a chuck portion 11 and at the same time a weight 13 is loaded on the tip portion of the golf club shaft 1. Then the tip portion of the golf club shaft 1 is vibrated in the vertical direction from the foregoing state and the frequency f1 (cpm) per 1 minute of the golf club shaft 1 is measured. Further, as shown in FIG. 8, the tip portion of the golf club shaft 1 is fastened to the chuck portion 11 and at the same time the weight 13 is loaded on the rear end portion of the golf club shaft 1. Then the rear end portion of the golf club shaft 1 is vibrated in the vertical direction from the foregoing state and the frequency f2 (cpm) per 1 minute of the golf club shaft 1 is measured. Then a ratio of both frequencies (f1/f2) is obtained. By obtaining this ratio of frequencies (f1/f2), bending performance of a golf club shaft which affects height of trajectory of a hit ball by a golf club, is obtained. Further, a sum of both frequencies (f1+f2) is obtained. By obtaining this sum of frequencies (f1+f2), variation of frequency value caused by a distribution of rigidity of the golf club shaft 1 is offset and effective flexibility of a golf club shaft is obtained.

In a method to measure frequencies in accordance with the present invention, a position in circumference direction where a golf club shaft is fastened to a device of measuring frequencies, is preferably kept constant or almost constant both in fastening a rear end portion and fastening a tip portion. It is easily kept constant by marking a line 31 on the golf club shaft as shown in FIG. 9 and by facing line 31 toward the same direction or almost same direction with respect to the device of measuring frequencies both in the case of fastening the rear end portion 101 as shown in FIG. 10 and in the case of fastening the tip portion 102 as shown in FIG. 11. The foregoing almost constant means that line 31 shown in FIG. 10 and FIG. 11 is deviated in circumference direction within 20 degree from the position facing right above, preferably within 10 degree, more preferably within 5 degree. Since there is a possibility that frequency value of a golf club shaft varies a bit depending on circumference directions due to variation of golf club shaft itself as a product, it is preferable to measure frequencies at the constant circumference direction or almost constant circumference direction as mentioned before.

As mentioned before, since frequency values possibly vary a bit in the circumference direction of a golf club shaft itself, there may be some difference in the ratio and the sum of frequencies between the case of measuring a golf club shaft as shown in FIG. 10 and FIG. 11 and the case of measuring the same golf club shaft rotating 90 degree in the circumference direction from the each position of FIG. 10 and FIG. 11 as shown in FIG. 12 and FIG. 13. Then, when a golf club shaft is fabricated to be a golf club, fastened position of golf club shafts is preferably kept constant. For more details, a golf club shaft shown in FIG. 9, which was measured with fastening methods as shown in FIG. 10 and FIG. 11, is preferably fastened at such a position that line 31 faces to the front or to almost front, in a front view which the golf club head 3 of a golf club 21 is placed according to the lie angle in a manner as face portion 103 is facing to the front as shown in FIG. 14. To reflecting measured value of a golf club shaft to a golf club, vibration direction of a golf club shaft 1, which is measured with a device of measuring frequencies 10 shown in FIG. 15, most preferably conforms to main bending direction of a golf club 21 during actual swing shown in FIG. 16. For that, it is understood that a golf club shaft 1, which was measured with fastening methods as shown in FIG. 10 and FIG. 11, should be fabricated to be a golf club 21 by fastening at the position shown in FIG. 14. The foregoing position facing to almost front means that deflection in circumference direction from the position that line 31 in FIG. 14 faces to the front, is within 15 degree, preferably within 10 degree, more preferably within 5 degree, furthermore preferably within 3 degree.

Further, in a simple golf club shaft, a logo mark 32 is marked by means of printing, etc., on the golf club shaft 1 in the same axle with line 31, as shown in FIG. 17 and the golf club shaft 1 is preferably fastened at the position that line 31 and logo mark 32 face to the front or to almost front in a front view which a golf club head of a golf club 21 is placed on plane 111 according to the lie angle, in a manner as face portion 103 is facing to the front as shown in FIG. 18. Moreover, as shown in FIG. 19, when the logo mark 32 is provided to the front in a view of golf club 21 from toe side, line 31 may be placed at the position deflecting 90 degree in circumference direction from the position of logo mark 32 at the stage of being a golf club shaft, as shown in FIG. 20.

As mentioned above, it was described that in measuring frequencies in FIG. 15, vibrating direction of a golf club shaft most preferably accords to main bending direction of the golf club during actual swing in FIG. 16. For example, a golf club shaft shown in FIG. 9, which was measured with fastening methods as shown in FIG. 10 and FIG. 11, is conceivably assembled to be a golf club as shown in FIG. 21. Specifically, vibrating direction of a golf club shaft is deflected at 90 degree from main bending direction of the golf club during actual swing. It is surely most preferable that vibrating direction of a golf club shaft accords to the main bending direction of the golf club during actual swing. But, to determine vibrating direction of a golf club shaft with a constant relation with main vending direction of the golf club during actual swing, is more preferable than to determine without a constant relation. In an actual conventional method to measure frequencies, as shown in FIG. 22, the measurement is mostly carried out in a manner of fastening a golf club 21 as toe portion 104 of the golf club 21 turns down. This means an example that vibration direction of a golf shaft is deflected at 90 degree from main bending direction of a golf club during actual swing.

Needless to say, line 31 used for determining direction in measuring frequencies as mentioned above may be hidden under a grip in a completed golf club. Line 31 may be used as a mark in measuring frequencies, and whether line 31 appears or is hidden in a golf club may be decided appropriately from a viewpoint of designing.

A tip portion of a golf club shaft in accordance with the present invention means an end portion where a golf club head is assembled, and a rear end portion means an end portion where a grip or a grip portion is assembled. In a golf club shown in FIG. 23, the end portion where grip 2 is assembled is denoted by a rear end portion 101 and the end portion where golf club head 3 is assembled, is denoted by tip portion 102. In typical golf club shaft 1, the rear end portion 101 where the grip 2 is assembled has bigger diameter than tip portion 102 where golf club head 3 is assembled. But as shown in FIG. 24, a golf club in which tip portion 102 where golf club head 3 is assembled has bigger diameter than rear end portion 101 where grip 2 is assembled, is conceivable.

Further a golf club where a golf club shaft 1 becomes partly grip portion 105 may exist as shown in FIG. 25. In this case, end portion to become grip portion 105 is denoted by rear end portion 101 and the other end portion where golf club head 3 is assembled is denoted by tip portion 102.

In the foregoing measurement of frequencies, the length to fasten a golf club shaft 1 is 178 mm, but, when it is in a range of 177.5 mm to 178.5 mm, frequencies obtained are substantially same. Accordingly, those are included in the present invention. Moreover, the mass of the weight 13 is set to 200 g, but, when the mass is in a range of 199.5 g to 200.5 g, frequencies obtained are substantially same. Accordingly, those are included in the present invention. Further, the loading length of weight 13 is set to 30 mm, but, when it is in a range of 29.5 mm to 30.5 mm, frequencies obtained are substantially same. Accordingly, those are included in the present invention.

Fastening length in the present invention is a distance (Da) from the end portion 121 to chuck 11a of chuck portion 11 when end surface 121 of a golf club shaft 1 is vertical to a golf club shaft axis 122 as shown in FIG. 26(a). Further, as shown in FIG. 26(b), when the end surface 121 is not vertical to the golf club shaft axis 122, fastening length is a distance (Db) from the most projected position of the end surface 121 to chuck 11a of chuck portion 11. Moreover, a fastening method may be a method to fasten by nipping from the upper and lower sides, a method to fasten with a drill chuck and the like, and the method is not limited as far as golf club shafts are fastened firmly.

The weight is one which can be firmly fixed on a golf club shaft and it may have cylindrical, rectangular, polygonal pillar shape and the like, but it is not particularly limited. Such sticky material having some weight as lead tape may be wounded on the golf club shaft. Preferably the center of gravity of the weight is located close to the golf club shaft axis. The center of gravity is preferably located numerically within 5 mm from the golf club axis in a fasten state of a golf club shaft.

As a structure of the weight, a drill chuck structure and the like may be conceivable to fasten golf club shafts having different diameter firmly. As other examples of the weight, as shown in FIG. 27, a weight tape 61 composed of lead, etc., may be conceivably wounded around a golf club shaft 1 to be fastened. The material of the weight tape is not particularly limited, but materials which can be fastened by winding around a golf club shaft are preferable. Structures of the weight tape are generally a plurality of layers composed of weight layers and sticky layers such as double-faced sticky tape. Shape of the tape is preferably rectangular same as typical tapes having small variation in width. Variation in width to longitudinal direction is preferably within 1 mm. When maximum width in longitudinal direction of weight tape 61 is denoted by Dx as shown in FIG. 28 (a), all lead tapes are preferably wounded within distance Dy (Dy≧Dx) from end surface 121, as shown in FIG. 28(b), satisfying a formula Dy≦Dx+5 mm, preferably satisfying a formula Dy≦Dx+3 mm.

In the foregoing golf club set, golf clubs having loft angles in a range of 16 degree to 41 degree is denoted by continuous natural number X starting from 1 in order of increasing loft angle from the lowest, and, in addition, the foregoing ratio of frequencies is denoted by Z. When the ratio Z of frequencies corresponding to natural number X of each golf clubs is plotted on coordinate axis X-Z, plots of all of the golf clubs having loft angle θ in a range of 16 degree to 41 degree become a straight line or almost straight line.

FIG. 29 is a graph showing a relation of natural number X corresponding to an order of the club number and ratio Z of frequencies. A shows a relation in an ideal golf club set in accordance with the present invention, and B shows a relation in a conventional golf club set. Specifically, in a conventional golf club set, the club number has no constant correlation with ratio of frequencies. However, since the club number has a constant correlation with ratio of frequencies in an ideal golf club set in accordance with the present invention, harmonized height of trajectory of a hit ball through a whole golf club set can be obtained.

More concretely, in golf clubs having loft angle θ in a range of 16 degree to 41 degree, when a distribution of ratio Z of frequencies to the natural number X is fitted on a regression line, the ratio Z of frequencies is determined so that estimated error to the regression line is 0.05 or less. What the estimated error is 0.05 or less means that the error between estimated value calculated by inputting natural number X, which is determined corresponding to the club number, and by inputting the ratio Z of frequencies in a function of the regression line and the ratio Z of frequencies, is 0.05 or less in the absolute value, that is, it indicates −0.05 or more and +0.05 or less. In this case estimated error is preferably 0.03 or less, more preferably 0.015 or less.

Slope of the foregoing regression line is not particularly limited, but by limiting the scope of the value, it is possible to constitute a golf club set meeting golfer's preference.

When the foregoing slope of a regression line is determined as −0.01 or less, preferably −0.3 or more and −0.01 or less, more preferably −0.25 or more and −0.02 or less, a golf club set in which height of trajectory of a hit ball by golf clubs having comparatively smaller loft angle θ becomes higher, may be fabricated. These golf club sets may be mainly suitable to golfers who want to get sufficient flying distance by heightening trajectory of a hit ball by golf clubs having smaller loft angle θ.

When the foregoing slope of a regression line is determined as −0.01 or more, preferably −0.01 or more and 0.2 or less, more preferably 0 or more and 0.15 or less, a golf club set in which height of trajectory of a hit ball by golf clubs having comparatively smaller loft angle θ becomes lower, may be fabricated. These golf club sets may be mainly suitable for golfers who want to get certain direction by lowering trajectory of a hit ball by golf clubs having smaller loft angle θ.

Effect of the foregoing slope of a regression line shows just general trends. Therefore, golfers can select a golf club set having specified value as a slope of the foregoing regression line considering own skill level, preferable bending of golf club shafts, feeling, preferable strategy, preferable feeling of hitting a ball and the like.

Adding to varying ratio Z of frequencies to natural number X linearly as described above, it is preferable to vary the sum Y of frequencies to natural number X linearly, wherein a sum (f1+f2) of a frequency f1 obtained by measuring in a state that rear end portion of a golf club shaft is fastened and a frequency f2 obtained by measuring in a state that the tip portion of the golf club shaft is fastened, is denoted by Y (cpm).

Specifically, in golf clubs having loft angle θ in a range of 16 degree to 41 degree, when a distribution of the sum Y of frequencies to the natural number X is fitted on a regression line, the sum Y of frequencies is preferably determined so that estimated error to the regression line is 30 cpm or less, preferably 20 cpm or less, more preferably 10 cpm or less. By determining Y as foregoing relations, harmonized height of trajectory of a hit ball is obtained more exactly through a whole golf club set.

Moreover, when, in the foregoing golf club set, using loft angle θ instead of natural number X, ratio Z of frequencies corresponding to loft angle θ of each golf club is plotted on θ−Z coordinate, the plots for all of the golf clubs having loft angle θ in a range of 16 degree to 41 degree become a straight line or almost straight line.

FIG. 30 is a graph showing a relation between loft angle θ and ratio Z of frequencies. A shows a relation in an ideal golf club set according to the present invention, and B shows a relation in conventional golf club set. Specifically, in a conventional golf club set, loft angle θ has no constant correlation with ratio of frequencies. However, since the loft angle θ has a constant correlation with ratio of frequencies in an ideal golf club set in accordance with the present invention, harmonized height of trajectory of a hit ball can be obtained through a whole golf club set.

More concretely, in golf clubs having loft angles θ in a range of 16 degree to 41 degree, when a distribution of ratio Z of frequencies to loft angle θ is fitted on a regression line, the ratio Z of frequencies is determined so that estimated error to the regression line is 0.05 or less. What the estimated error is 0.05 or less means that the error between estimated values calculated by inputting loft angle θ of the golf club and the ratio Z of frequencies in a function of the regression line and the ratio Z of frequencies, is 0.05 or less in the absolute value, that is, it indicates −0.05 or more and +0.05 or less. In this case estimated error is preferably 0.03 or less, more preferably 0.015 or less.

Slope of the foregoing regression line is not particularly limited, but, by limiting the scope of the value, it is possible to constitute a golf club set meeting golfer's preference.

When the foregoing slope of a regression line is determined as −0.0025 or less, preferably −0.075 or more and −0.0025 or less, more preferably −0.0625 or more and −0.005 or less, a golf club set in which height of trajectory of a hit ball by golf clubs having comparatively smaller loft angle θ becomes higher, may be fabricated. These golf club sets may be mainly suitable for golfers who want to get sufficient flying distance by heightening trajectory of a hit ball by golf clubs having smaller loft angle θ.

When the foregoing slope of a regression line is determined as −0.0025 or more, preferably −0.0025 or more and 0.05 or less, more preferably 0 or more and 0.0375 or less, a golf club set in which height of trajectory of a hit ball by golf clubs having comparatively smaller loft angle θ becomes lower, may be fabricated. These golf club sets may be mainly suitable for golfers who want to get certain direction by lowering trajectory of a hit ball by golf clubs having smaller loft angle θ.

Effect of the foregoing slope of a regression line shows just general trends. Therefore, golfers can select a golf club set having specified value as a slope of the foregoing regression line, considering own skill level, preferable bending of golf club shafts, feeling, preferable strategy, preferable feeling of hitting a ball and the like.

Adding to varying ratio Z of frequencies to a loft angle θ linearly as described above, it is preferable to vary the sum Y of frequencies to a loft angle θ linearly, wherein a sum (f1+f2) of a frequency f1 obtained by measuring in a state that a rear end portion of a golf club shaft is fastened and a frequency f2 obtained by measuring in a state that a tip portion of the golf club shaft is fastened, is denoted by Y (cpm).

Specifically, in golf clubs having loft angles θ in a range of 16 degree to 41 degree, when a distribution of the sum Y of frequencies to a loft angle θ is fitted on a regression line, the sum Y of frequencies is preferably determined so that estimated error to the regression line is 30 cpm or less, preferably 20 cpm or less, more preferably 10 cpm or less. By determining Y as foregoing relations, harmonized height of trajectory of a hit ball is obtained more exactly through a whole golf club set.

In the foregoing golf club set, golf club shafts to be assembled to golf clubs having loft angles in a range of 16 degree to 41 degree is denoted by continuous natural number X starting from 1 in order from the longest golf club shaft, and, in addition, the foregoing ratio of frequencies is denoted by Z. When the ratio Z of frequencies corresponding to natural number X of each golf club shaft is plotted on X-Z coordinate, plots of all of the golf club shafts to be assembled to golf clubs having loft angle θ in a range of 16 degree to 41 degree become a straight line or almost straight line.

In a golf club set, in general, the larger the club number is, the shorter shaft length the golf club has. Therefore, the relations between natural number X and ratio Z of frequencies in a golf club shaft set may be determined in the same way as the foregoing golf club set.

Moreover, when, in the foregoing golf club set, using golf club shaft length L instead of natural number X, ratio Z of frequencies corresponding to length L of each golf club shaft is plotted on L-Z coordinate, the plots for all of the golf club shafts to be assembled to golf clubs having loft angle θ in a range of 16 degree to 41 degree become a straight line or almost straight line.

FIG. 31 is a graph showing a relation between golf club shaft length L and ratio Z of frequencies. A shows a relation in an ideal golf club set according to the present invention, and B shows a relation in conventional golf club set. Specifically, in a conventional golf club set, golf club shaft length has no constant correlation with ratio of frequencies. However, since golf club shaft length has a constant correlation with ratio of frequencies in an ideal golf club set in accordance with the present invention, harmonized height of trajectory of a hit ball can be obtained through a whole golf club set.

More concretely, in golf club shafts to be assembled to golf clubs having loft angle θ in a range of 16 degree to 41 degree, when a distribution of ratio Z of frequencies to golf club shaft length L is fitted on a regression line, the ratio Z of frequencies is determined so that estimated error to the regression line is 0.05 or less. What the estimated error is 0.05 or less means that the error between estimated value calculated by inputting golf club shaft length L and by inputting the ratio Z of frequencies in a function of the regression line and the ratio Z of frequencies, is 0.05 or less in the absolute value, that is, it indicates −0.05 or more and +0.05 or less. In this case, the estimated error is preferably 0.03 or less, more preferably 0.015 or less.

The above relationship can be maintained for golf club shafts to be assembled to golf clubs having loft angle θ out of the range of 16 degree to 41 degree. For example, the above relationship can be maintained for the entire golf club shaft set.

Slope of the foregoing regression line is not particularly limited, but, by limiting the scope of the value, it is possible to constitute a golf club set meeting golfer's preference.

When the foregoing slope of a regression line is determined as 0.00077 or more, preferably 0.00077 or more and 0.0231 or less, more preferably 0.00154 or more and 0.01925 or less, a golf club set in which height of trajectory of a hit ball by golf clubs having comparatively longer golf club shaft length L becomes higher, may be fabricated. These golf club sets may be mainly suitable for a type of golfers who want to get sufficient flying distance by heightening trajectory of a hit ball by golf clubs having longer golf club shaft length L.

When the foregoing slope of a regression line is determined as 0.00077 or less, preferably −0.0154 or more and 0.0077 or less, more preferably −0.01155 or more and 0 or less, a golf club set in which height of trajectory of a hit ball by golf clubs having comparatively longer golf club shaft length L becomes lower, may be fabricated. These golf club sets may be mainly suitable for a type of golfers who want to get certain direction by lowering trajectory of a hit ball by golf clubs having longer golf club shaft length L.

Effect of the foregoing slope of a regression line shows just general trends. Therefore, golfers can select a golf club set having specified value as a slope of the foregoing regression line, considering own skill level, preferable bending of golf club shafts, feeling, preferable strategy, preferable feeling of hitting a ball and the like.

Adding to varying ratio Z of frequencies to golf club shaft length L linearly as described above, it is preferable to vary the sum Y of frequencies to golf club shaft length L linearly, wherein a sum (f1+f2) of a frequency f1 obtained by measuring in a state that a rear end portion of a golf club shaft is fastened and a frequency f2 obtained by measuring in a state that a tip portion of the golf club shaft is fastened, is denoted by Y (cpm).

Specifically, in golf club shafts to be assemble to golf clubs having loft angle θ in a range of 16 degree to 41 degree, when a distribution of the sum Y of frequencies to length L is fitted on a regression line, the sum Y of frequencies is preferably determined so that estimated error to the regression line is 30 cpm or less, preferably 20 cpm or less, more preferably 10 cpm or less. By determining Y as the foregoing relations, harmonized height of trajectory of a hit ball is obtained more exactly through a whole golf club set.

In the foregoing golf club set, golf clubs having loft angles in a range of 16 degree to 41 degree is denoted by continuous natural number X starting from 1 in order from the club number having the lowest loft angle and, in addition, the foregoing sum of frequencies is denoted by Y (cpm). When the sum Y of frequencies corresponding to natural number X of each golf club is plotted on X-Y coordinate, plots of all of the golf clubs having loft angle θ in a range of 16 degree to 41 degree become a straight line or almost straight line.

FIG. 32 is a graph showing a relation between natural number X corresponding to order of the club number and the sum Y of frequencies. A shows a relation in an ideal golf club set in accordance with the present invention, and B shows a relation in conventional golf club set. Specifically, in a conventional golf club set, the club number has no constant correlation with the sum of frequencies. However, since the club number has a constant correlation with the sum of frequencies in an ideal golf club set in accordance with the present invention, harmonized flexibility of golf club shafts can be obtained through a whole golf club set.

More concretely, in golf clubs having loft angle θ in a range of 16 degree and 41 degree, the sum Y of frequencies is determined to natural number X in a scope of satisfying the following formula,
aX+b≦Y≦aX+b+12  (1)
where coefficients a and b are arbitrary constants.

Specifically, the sum Y of frequencies is contained in a scope between two parallel straight lines, Y=aX+b and Y=aX+b+12, more preferably contained in a scope between Y=aX+b and Y=aX+b+9, further more preferably contained in a scope between Y=aX+b and Y=aX+b+6. In the present invention, for golf clubs satisfying a formula, 16≦θ≦41, at least one combination of coefficients a and b preferably exists so that all plots of the sum Y of frequencies plotted to natural number X are contained in the scope between the foregoing two straight lines.

The above coefficient a is not particularly limited, but by limiting the range of the value, it is possible to constitute a golf club set in accordance with golfer's preference.

When the coefficient a is 24 or less, preferably 0 or more and 24 or less, more preferably 4 or more and 20 or less, a golf club set in which golf club shafts of golf clubs having lower loft angle θ are stiffer, is fabricated. These golf club sets are mainly suitable for a type of golfers who want to get flying distance by swinging with stronger power in clubs having lower loft angle θ.

When the coefficient a is 24 or more, preferably 24 or more and 48 or less, more preferably 28 or more and 44 or less, a golf club set in which golf club shafts of golf clubs having lower loft angle θ are more flexible, is fabricated. These golf club sets are mainly suitable for a type of golfers who want to get certainly flying distance corresponding to the club number by swinging with effective use of the length of club and with easy feeling in clubs having lower loft angle θ.

Effect of the foregoing coefficient a shows just general trends. Therefore, golfers can select a golf club set having specified coefficient a, considering own skill level, preferable bending of golf club shafts, feeling, preferable strategy, preferable feeling of hitting a ball and the like.

Besides specifying linear variation of the sum Y of frequencies using 2 lines with natural number X as a variable as described above, linear variation of the sum Y of frequencies may be specified by using a regression line of all plots of the sum Y of frequencies plotted to natural number X.

Specifically, in golf clubs having loft angle θ in a range of 16 degree to 41 degree, when a distribution of the sum Y of frequencies to natural number X is fitted on a regression line, the sum Y of frequencies is determined so that estimated error to the regression line is 8 (cpm) or less. What the estimated error is 8 (cpm) or less means that the error between estimated value calculated by inputting natural number X corresponding to the club number and the sum Y of frequencies in a function of the regression line and the sum Y of frequencies, is 8 (cpm) or less in the absolute value, that is, it indicates −8 (cpm) or more and +8 (cpm) or less. In this case estimated error is preferably 6 (cpm) or less, more preferably 4 (cpm) or less.

The above slope of a regression line of the sum Y of frequencies to natural number X is not particularly limited, but by limiting the range of the value, it is possible to constitute a golf club set in accordance with golfer's preference.

When the foregoing slope is 24 or less, preferably 0 or more and 24 or less, more preferably 4 or more and 20 or less, a golf club set in which golf club shafts of golf clubs having lower loft angle θ are stiffer, is fabricated. These golf club sets are mainly suitable for a type of golfers who want to get flying distance by swinging with stronger power in clubs having lower loft angle θ.

When the foregoing slope is 24 or more, preferably 24 or more and 48 or less, more preferably 28 or more and 44 or less, a golf club set in which golf club shafts of golf clubs having lower loft angle θ are more flexible, is fabricated. These golf club sets are mainly suitable for a type of golfers who want to get certainly flying distance corresponding to the club number by swinging with effective use of the length of club and with easy feeling in clubs having lower loft angle θ.

Effect of the foregoing slope shows just general trends. Therefore, golfers can select a golf club set having specified slope of the regression line, considering own skill level, preferable bending of golf club shafts, feeling, preferable strategy, preferable feeling of hitting a ball and the like.

Adding to varying the sum Y of frequencies to natural number X linearly as described above, it is preferable to vary the ratio Z of frequencies to natural number X linearly, wherein ratio (f1/f2) of a frequency f1 obtained by measuring in a state that a rear end portion of a golf club shaft is fastened and a frequency f2 obtained by measuring in a state that a tip portion of the golf club shaft is fastened, is denoted by Z.

Specifically, golf clubs having loft angle θ in a range of 16 degree to 41 degree, when a distribution of ratio Z of frequencies to natural number X is fitted on a regression line, the ratio Z of frequencies is preferably determined so that an estimated error to the regression line is 0.15 or less, preferably 0.1 or less, more preferably 0.05 or less. By determining Z as the foregoing relations, harmonized flexibility of golf club shafts is obtained more exactly through a whole golf club set.

Moreover, when in the foregoing golf club set, using loft angle θ instead of natural number X, the sum Y of frequencies corresponding to loft angle θ of each golf club is plotted on θ-Y coordinates, the plots for all of the golf clubs having loft angle θ in a range of 16 degree to 41 degree become a straight line or almost straight line.

FIG. 33 is a graph showing a relation between loft angle θ and the sum Y of frequencies. A shows a relation in an ideal golf club set according to the present invention, and B shows a relation in conventional golf club set. Specifically, in a conventional golf club set, loft angle θ has no constant correlation with the sum of frequencies. However, since loft angle θ has a constant correlation with the sum of frequencies in an ideal golf club set in accordance with the present invention, harmonized flexibility of golf club shaft can be obtained through a whole golf club set.

More concretely in golf clubs having loft angles in a range of 16 degree to 41 degree, the sum Y of frequencies is determined to loft angle θ in a scope satisfying the following formula (2),
cθ+d≦Y≦cθ+d+12  (2)
where coefficients c and d are arbitrary constants.

Specifically, the sum Y of frequencies is contained in a scope between two parallel straight lines, Y=cθ+d and Y=cθ+d+12, more preferably contained in a scope between Y=cθ+d and Y=cθ+d+9, further more preferably contained in a scope between Y=cθ+d and Y=cθ+d+6. In the present invention, for golf clubs satisfying a formula, 16≦θ≦41, at least one combination of coefficients c and d preferably exists so that all plots of the sum Y of frequencies plotted to loft angle θ are contained in the scope between the foregoing two straight lines.

The above coefficient c is not particularly limited, but, by limiting the range of the value, it is possible to constitute a golf club set in accordance with golfer's preference.

When the coefficient c is 6 or less, preferably 0 or more and 6 or less, more preferably 1 or more and 5 or less, a golf club set in which golf club shafts of golf clubs having comparatively lower loft angle θ are stiffer, is fabricated. These golf club sets are mainly suitable for a type of golfers who want to get flying distance by swinging with stronger power in clubs having lower loft angle θ.

When the coefficient c is 6 or more, preferably 6 or more and 12 or less, more preferably 7 or more and 11 or less, a golf club set in which golf club shafts of golf clubs having comparatively lower loft angle θ are more flexible, is fabricated. These golf club sets are mainly suitable for a type of golfers who want to get certainly flying distance corresponding to the club number by swinging with effective use of the length of club and with easy feeling in clubs having lower loft angle θ.

Effect of the foregoing coefficient c shows just general trends. Therefore, golfers can select a golf club set having specified coefficient c, considering own skill level, preferable bending of golf club shafts, feeling, preferable strategy, preferable feeling of hitting a ball and the like.

Besides specifying linear variation of the sum Y of frequencies using two lines with loft angle θ as a variable, linear variation of the sum Y of frequencies may be specified by using a regression line of all plots of the sum Y of frequencies plotted to loft angle θ.

Specifically, in golf clubs having loft angle θ in a range of 16 degree to 41 degree, when a distribution of the sum Y of frequencies to loft angle θ is fitted on a regression line, the sum Y of frequencies is determined so that estimated error to the regression line is 8 (cpm) or less. What the estimated error is 8 (cpm) or less means that the error between estimated value calculated by inputting loft angle θ of golf clubs and the sum Y of frequencies in a function of the regression line and the sum Y of frequencies, is 8 (cpm) or less in the absolute value, that is, it indicates −8 (cpm) or more and +8 or less. In this case estimated error is preferably 6 (cpm) or less, more preferably 4 (cpm) or less.

The above slope of a regression line of the sum Y of frequencies to loft angle θ is not particularly limited, but, by limiting the range of the value, it is possible to constitute a golf club set in accordance with golfer's preference.

When the foregoing slope is 6 or less, preferably 0 or more and 6 or less, more preferably 1 or more and 5 or less, a golf club set in which golf club shafts of golf clubs having comparatively lower loft angle θ are stiffer, is fabricated. These golf club sets are mainly suitable for a type of golfers who want to get flying distance by swinging with stronger power in clubs having lower loft angle θ.

When the foregoing slope is 6 or more, preferably 6 or more and 12 or less, more preferably 7 or more and 11 or less, a golf club set in which golf club shafts of golf clubs having comparatively lower loft angle θ are more flexible, is fabricated. These golf club sets are mainly suitable for a type of golfers who want to get certainly flying distance corresponding to the club number by swinging with effective use of the length of clubs and with easy feeling in clubs having lower loft angle θ.

Effect of the foregoing slope shows just general trends. Therefore, golfers can select a golf club set having specified slope of the regression line, considering own skill level, preferable bending of golf club shafts, feeling, preferable strategy, preferable feeling of hitting a ball and the like.

Adding to varying the sum Y of frequencies to loft angle θ linearly as described above, it is preferable to vary the ratio Z of frequencies to loft angle θ linearly, wherein ratio (f1/f2) of a frequency f1 obtained by measuring in a state that a rear end portion of a golf club shaft is fastened and a frequency f2 obtained by measuring in a state that a tip portion of the golf club shaft is fastened, is denoted by Z.

Specifically, in golf clubs having loft angle θ in a range of 16 degree to 41 degree, when a distribution of ratio Z of frequencies to loft angle θ is fitted on a regression line, the ratio Z of frequencies is preferably determined so that estimated error to the regression line is 0.15 or less, preferably 0.1 or less, more preferably 0.05 or less. By determining Z as foregoing relations, harmonized flexibility of golf club shafts can be obtained more exactly through a whole golf club set.

In the foregoing golf club set, when golf club shafts to be assembled to golf clubs having loft angles in a range of 16 degree to 41 degree is denoted by continuous natural number X starting from 1 in order from clubs having the longest golf club shaft length, and, in addition, the foregoing sum of frequencies is denoted by Y (cpm). When the sum Y of frequencies corresponding to natural number X of each golf club is plotted on X-Y coordinate, plots of all of the golf club shafts to be assembled to golf clubs having loft angle θ in a range of 16 degree to 41 degree become a straight line or almost straight line.

In a golf club set, in general, the larger the club number is, the shorter length the golf club shaft has. Then the relations between natural number X and the sum Y of frequencies in a golf club shaft set may be determined in the same way as the foregoing golf club set.

Moreover, when, in the foregoing golf club set, using golf club shaft length L instead of natural number X, the sum Y of frequencies corresponding to length L of each golf club shaft is plotted on L-Y coordinate, the plots for all of the golf club shafts to be assembled to golf clubs having loft angle θ in a range of 16 degree to 41 degree become a straight line or almost straight line.

FIG. 34 is a graph showing a relation between golf club shaft length L and the sum Y of frequencies. A shows a relation in an ideal golf club set, and B shows a relation in conventional golf club set. Specifically, in a conventional golf club set, golf club shaft length has no constant correlation with the sum of frequencies. However, since golf club shaft length has a constant correlation with the sum of frequencies in an ideal golf club set in accordance with the present invention, harmonized flexibility of golf club shafts can be obtained through a whole golf club set.

More concretely, in golf club shafts to be assembled to golf clubs having loft angle θ in a range of 16 degree to 41 degree, when a distribution of the sum Y of frequencies to golf club shaft length L is fitted on a regression line, the sum Y of frequencies is determined so that estimated error to the regression line is 8 (cpm) or less. What the estimated error is 8 (cpm) or less means that the error between estimated value calculated by inputting golf club shaft length L and by inputting the sum Y of frequencies in a function of the regression line and the sum Y of frequencies, is 8 (cpm) or less in the absolute value, that is, it indicates −8 (cpm) or more and +8 (cpm) or less. In this case estimated error is preferably 6 (cpm) or less, more preferably 4 (cpm) or less.

The above relationship can be maintained for golf club shafts to be assembled to golf clubs having loft angle θ out of the range of 16 degree to 41 degree. For example, the above relationship can be maintained for the entire golf club shaft set.

The above slope of a regression line of the sum Y of frequencies to golf club shaft length L is not particularly limited, but, by limiting the range of the value, it is possible to constitute a golf club set in accordance with golfer's preference.

When the foregoing slope is −1.85 or more, preferably −1.85 or more and 0 or less, more preferably −1.55 or more and −0.3 or less, a golf club set in which golf club shafts of golf clubs having comparatively longer golf club shaft length L are stiffer, is fabricated. These golf club sets are mainly suitable for a type of golfers who want to get flying distance by swinging with stronger power in clubs having longer golf club shaft length L.

When the foregoing slope is −1.85 or less, preferably −3.7 or more and −1.85 or less, more preferably −3.4 or more and −2.15 or less, a golf club set in which golf club shafts of golf clubs having comparatively longer golf club shaft length L are more flexible, is fabricated. These golf club sets are mainly suitable for a type of golfers who want to get certainly flying distance corresponding to the club number by swinging with effective use of the length of clubs and with easy feeling in clubs having longer golf club shaft length L.

Effect of the foregoing slope shows just general trends. Therefore, golfers can select a golf club set having specified slope, considering own skill level, preferable bending of golf club shafts, feeling, preferable strategy, preferable feeling of hitting a ball and the like.

Adding to varying the sum Y of frequencies to golf club shaft length L linearly as described above, it is preferable to vary the ratio Z of frequencies to golf club shaft length L linearly, wherein ratio (f1/f2) of a frequency f1 obtained by measuring in a state that a rear end portion of a golf club shaft is fastened and a frequency f2 obtained by measuring in a state that a tip portion of the golf club shaft is fastened, is denoted by Z.

Specifically, in golf club shafts to be assembled to golf clubs having loft angle θ in a range of 16 degree to 41 degree, when a distribution of ratio Z of frequencies to length L is fitted on a regression line, the ratio Z of frequencies is preferably determined so that estimated error to the regression line is 0.15 or less, preferably 0.1 or less, more preferably 0.05 or less. By determining Z as the foregoing relations, harmonized flexibility of golf club shafts can be obtained more exactly through a whole golf club set.

The foregoing constituents of the present invention provide remarkable effects particularly when they are applied to a golf club set by use of golf club shafts made of fiber reinforced plastics.

Golf club shafts made of fiber reinforced plastics have more freedom in designing such that kinds of reinforced fiber and orient direction of fibers can be freely selected and rigidity distribution in golf club shafts can be varied in longitudinal direction, than golf club shafts made of metal. In particular, lately length of golf club has become longer and accompanying with the trend, variation of rigidity distribution in golf club shafts has become bigger. Therefore in the case of golf club shafts made of fiber reinforced plastic, when a golf club set is designed based on conventional yardstick so that height of trajectory of a hit ball by the golf clubs can be harmonized among the club numbers, it was very difficult to obtain harmony in height of trajectory of a hit ball actually by the golf clubs among the club numbers.

On the contrary, in the present invention, even when golf club shafts are made of fiber reinforced plastics, a golf club set which can harmonize actually height of trajectory of a hit ball by golf clubs among the club numbers, can be easily constituted.

Further, in the case of golf club shafts made of fiber reinforced plastics, even when a golf club set is designed based on conventional yardstick so that flexibility of golf club shafts can be harmonized among the club numbers, it was very difficult to obtain harmony in flexibility felt actually by a person among the club numbers.

On the contrary, in the present invention, even when golf club shafts are made of fiber reinforced plastics, a golf club set in which flexibility of golf club shafts felt actually by a person, is harmonized among the club numbers, can be easily constituted.

A golf club set in the present invention comprises a plurality of golf clubs having variously different loft angles such as an iron golf club set, a wood golf club set, a golf club set including wood golf clubs and iron golf clubs, a golf club set including only ones corresponding to a long iron, a golf club set including utility golf clubs having middle performances between an wood golf club and an iron golf club, a golf club set comprised of golf clubs which are not classified in a wood golf club or a iron golf club.

EXAMPLE

In a golf club set comprising a plurality of golf clubs having variously different loft angles, golf club sets comprising golf club shafts having variously different frequency performance are fabricated as shown in example 1 to 18 and comparative example 1 to 2. In these golf club sets, golf clubs having the same loft angles are assembled with the same golf club head and the same grip. With regard to club length, the longest golf club (#3) is 39.0 inches and the length is shorten by 0.5 inches each in order of increasing club number and the shortest golf club (#8) is 36.5 inches. As the above golf club shafts, golf club shafts made of fiber reinforced plastics were used.

In Table 1 to Table 20, club number, natural number X, loft angle θ (degree), golf club shaft length L (mm), frequency f1 (cpm), frequency f2 (cpm), ratio Z of frequencies of golf club sets in example 1 to 18 and comparative example 1 to 2 are shown. Here, frequency f1 is a frequency, the frequency being measured by vibrating a tip portion of a golf club shaft in a state that a rear end portion is fastened for a length of 178 mm from the rear end and a 200 g weight is loaded on a tip portion for a length of 30 mm from the tip end. Frequency f2 is a frequency, the frequency being measured by vibrating the rear end portion of a golf club shaft in a state that the tip portion is fastened for a length of 178 mm from the tip end and a 200 g weight is loaded on the rear portion for a length of 30 mm from the rear end. The ratio Z of frequencies is a ratio (f1/f2) of frequency f1 to frequency f2.

TABLE 1
Example 1
			Length of
			golf club	Frequency	Frequency		Launching
	Natural	Loft angle θ	shaft	f1	f2	Ratio of	angle
Club #	number X	(degree)	L (mm)	(cpm)	(cpm)	frequencies Z	(degree)
# 3	1	20	962	549	201	2.731	16.6
# 4	2	24	949	548	224	2.446	18.6
# 5	3	28	936	545	251	2.171	20.5
# 6	4	32	923	540	285	1.895	22.4
# 7	5	36	910	532	326	1.632	24.2
# 8	6	40	897	506	378	1.339	25.9

TABLE 2
Example 2
			Length of
			golf club	Frequency	Frequency		Launching
	Natural	Loft angle θ	shaft	f1	f2	Ratio of	angle
Club #	number X	(degree)	L (mm)	(cpm)	(cpm)	frequencies Z	(degree)
# 3	1	20	962	632	227	2.784	16.4
# 4	2	24	949	657	252	2.607	18.6
# 5	3	28	936	660	283	2.332	20.5
# 6	4	32	923	672	326	2.061	22.2
# 7	5	36	910	677	367	1.845	24.3
# 8	6	40	897	697	421	1.656	26.8

TABLE 3
Example 3
			Length of
			golf club	Frequency	Frequency		Launching
	Natural	Loft angle θ	shaft	f1	f2	Ratio of	angle
Club #	number X	(degree)	L (mm)	(cpm)	(cpm)	frequencies Z	(degree)
# 3	1	20	962	550	256	2.148	16.2
# 4	2	24	949	571	306	1.866	18.3
# 5	3	28	936	588	354	1.661	20.5
# 6	4	32	923	592	423	1.400	22.2
# 7	5	36	910	593	509	1.165	24.3
# 8	6	40	897	594	636	0.934	26.1

TABLE 4
Example 4
			Length of
			golf club	Frequency	Frequency		Launching
	Natural	Loft angle θ	shaft	f1	f2	Ratio of	angle
Club #	number X	(degree)	L (mm)	(cpm)	(cpm)	frequencies Z	(degree)
# 3	1	20	962	472	193	2.446	16.5
# 4	2	24	949	506	229	2.210	18.6
# 5	3	28	936	532	269	1.978	20.6
# 6	4	32	923	551	323	1.706	22.3
# 7	5	36	910	568	387	1.468	24.3
# 8	6	40	897	571	463	1.233	26.2

TABLE 5
Example 5
			Length of
			golf club	Frequency	Frequency		Launching
	Natural	Loft angle θ	shaft	f1	f2	Ratio of	angle
Club #	number X	(degree)	L (mm)	(cpm)	(cpm)	frequencies Z	(degree)
# 3	1	20	962	411	208	1.976	16.5
# 4	2	24	949	409	224	1.826	18.3
# 5	3	28	936	405	237	1.709	20.3
# 6	4	32	923	403	254	1.587	22.3
# 7	5	36	910	398	270	1.474	24.3
# 8	6	40	897	388	288	1.347	26.2

TABLE 6
Example 6
			Length of
			golf club	Frequency	Frequency		Launching
	Natural	Loft angle θ	shaft	f1	f2	Ratio of	angle
Club #	number X	(degree)	L (mm)	(cpm)	(cpm)	frequencies Z	(degree)
# 3	1	20	962	358	203	1.764	15.9
# 4	2	24	949	365	212	1.722	17.8
# 5	3	28	936	390	222	1.757	20.3
# 6	4	32	923	405	231	1.753	22.6
# 7	5	36	910	409	241	1.697	24.4
# 8	6	40	897	416	251	1.657	26.3

TABLE 7
Example 7
			Length of
			golf club	Frequency	Frequency		Launching
	Natural	Loft angle θ	shaft	f1	f2	Ratio of	angle
Club #	number X	(degree)	L (mm)	(cpm)	(cpm)	frequencies Z	(degree)
# 3	1	20	962	384	189	2.032	16.4
# 4	2	24	949	399	197	2.025	18.6
# 5	3	28	936	403	205	1.966	20.4
# 6	4	32	923	415	213	1.948	22.5
# 7	5	36	910	420	221	1.900	24.4
# 8	6	40	897	438	230	1.904	26.8

TABLE 8
Example 8
			Length of
			golf club	Frequency	Frequency		Launching
	Natural	Loft angle θ	shaft	f1	f2	Ratio of	angle
Club #	number X	(degree)	L (mm)	(cpm)	(cpm)	frequencies Z	(degree)
# 3	1	20	962	481	351	1.370	16.1
# 4	2	24	949	499	366	1.363	18.3
# 5	3	28	936	503	382	1.317	20.1
# 6	4	32	923	514	398	1.291	22.2
# 7	5	36	910	524	416	1.260	24.2
# 8	6	40	897	533	434	1.228	26.1

TABLE 9
Example 9
			Length of
			golf club	Frequency	Frequency		Launching
	Natural	Loft angle θ	shaft	f1	f2	Ratio of	angle
Club #	number X	(degree)	L (mm)	(cpm)	(cpm)	frequencies Z	(degree)
# 3	1	20	962	378	284	1.331	16.1
# 4	2	24	949	381	292	1.305	18.0
# 5	3	28	936	396	301	1.316	20.2
# 6	4	32	923	400	310	1.290	22.1
# 7	5	36	910	405	319	1.270	24.0
# 8	6	40	897	415	328	1.265	26.2

TABLE 10
Comparative example 1
			Length of
			golf club	Frequency	Frequency		Launching
	Natural	Loft angle θ	shaft	f1	f2	Ratio of	angle
Club #	number X	(degree)	L (mm)	(cpm)	(cpm)	frequencies Z	(degree)
# 3	1	20	962	401	201	1.995	17.1
# 4	2	24	949	408	242	1.686	17.9
# 5	3	28	936	415	256	1.621	20.3
# 6	4	32	923	422	287	1.470	22.0
# 7	5	36	910	429	305	1.407	24.6
# 8	6	40	897	436	369	1.182	25.0

TABLE 11
Example 10
			Length of
			golf club	Frequency	Frequency		Launching
	Natural	Loft angle θ	shaft	f1	f2	Ratio of	angle
Club #	number X	(degree)	L (mm)	(cpm)	(cpm)	frequencies Z	(degree)
# 3	1	20	962	332	269	1.234	16.0
# 4	2	24	949	351	280	1.254	18.2
# 5	3	28	936	362	294	1.231	20.0
# 6	4	32	923	380	307	1.238	22.2
# 7	5	36	910	392	321	1.221	24.0
# 8	6	40	897	409	334	1.225	26.2

TABLE 12
Example 11
			Length of
			golf club	Frequency	Frequency		Launching
	Natural	Loft angle θ	shaft	f1	f2	Ratio of	angle
Club #	number X	(degree)	L (mm)	(cpm)	(cpm)	frequencies Z	(degree)
# 3	1	20	962	413	307	1.345	16.3
# 4	2	24	949	415	314	1.322	18.2
# 5	3	28	936	429	313	1.371	20.3
# 6	4	32	923	433	311	1.392	22.4
# 7	5	36	910	434	326	1.331	23.6
# 8	6	40	897	445	328	1.357	25.8

TABLE 13
Example 12
			Length of
			golf club	Frequency	Frequency		Launching
	Natural	Loft angle θ	shaft	f1	f2	Ratio of	angle
Club #	number X	(degree)	L (mm)	(cpm)	(cpm)	frequencies Z	(degree)
# 3	1	20	962	370	208	1.779	16.3
# 4	2	24	949	382	212	1.802	18.4
# 5	3	28	936	390	217	1.797	20.3
# 6	4	32	923	396	222	1.784	22.2
# 7	5	36	910	411	225	1.827	24.5
# 8	6	40	897	418	233	1.794	26.1

TABLE 14
Example 13
			Length of
			golf club	Frequency	Frequency		Launching
	Natural	Loft angle θ	shaft	f1	f2	Ratio of	angle
Club #	number X	(degree)	L (mm)	(cpm)	(cpm)	frequencies Z	(degree)
# 3	1	20	962	433	227	1.907	16.2
# 4	2	24	949	442	228	1.939	18.4
# 5	3	28	936	446	230	1.939	20.4
# 6	4	32	923	447	230	1.943	22.4
# 7	5	36	910	456	234	1.949	24.4
# 8	6	40	897	461	237	1.945	26.3

TABLE 15
Example 14
			Length of
			golf club	Frequency	Frequency		Launching
	Natural	Loft angle θ	shaft	f1	f2	Ratio of	angle
Club #	number X	(degree)	L (mm)	(cpm)	(cpm)	frequencies Z	(degree)
# 3	1	20	962	356	237	1.502	16.2
# 4	2	24	949	372	238	1.563	18.2
# 5	3	28	936	396	241	1.643	20.3
# 6	4	32	923	419	243	1.724	22.5
# 7	5	36	910	436	245	1.780	24.4
# 8	6	40	897	457	248	1.843	26.4

TABLE 16
Example 15
			Length of
			golf club	Frequency	Frequency		Launching
	Natural	Loft angle θ	shaft	f1	f2	Ratio of	angle
Club #	number X	(degree)	L (mm)	(cpm)	(cpm)	frequencies Z	(degree)
# 3	1	20	962	401	298	1.346	16.3
# 4	2	24	949	407	279	1.459	18.1
# 5	3	28	936	417	259	1.610	20.3
# 6	4	32	923	424	235	1.804	22.9
# 7	5	36	910	436	231	1.887	24.5
# 8	6	40	897	448	220	2.036	26.6

TABLE 17
Example 16
			Length of
			golf club	Frequency	Frequency		Launching
	Natural	Loft angle θ	shaft	f1	f2	Ratio of	angle
Club #	number X	(degree)	L (mm)	(cpm)	(cpm)	frequencies Z	(degree)
# 3	1	20	962	305	280	1.089	16.1
# 4	2	24	949	332	269	1.234	18.3
# 5	3	28	936	354	265	1.336	20.0
# 6	4	32	923	392	263	1.490	22.2
# 7	5	36	910	420	257	1.634	24.3
# 8	6	40	897	455	253	1.798	26.7

TABLE 18
Example 17
			Length of
			golf club	Frequency	Frequency		Launching
	Natural	Loft angle θ	shaft	f1	f2	Ratio of	angle
Club #	number X	(degree)	L (mm)	(cpm)	(cpm)	frequencies Z	(degree)
# 3	1	20	962	359	229	1.568	16.3
# 4	2	24	949	375	222	1.689	18.3
# 5	3	28	936	395	216	1.829	20.4
# 6	4	32	923	411	210	1.957	22.4
# 7	5	36	910	434	205	2.117	24.6
# 8	6	40	897	455	202	2.252	26.7

TABLE 19
Example 18
			Length of
			golf club	Frequency	Frequency		Launching
	Natural	Loft angle θ	shaft	f1	f2	Ratio of	angle
Club #	number X	(degree)	L (mm)	(cpm)	(cpm)	frequencies Z	(degree)
# 3	1	20	962	403	322	1.252	16.1
# 4	2	24	949	422	297	1.421	18.2
# 5	3	28	936	446	278	1.604	20.4
# 6	4	32	923	462	264	1.750	22.3
# 7	5	36	910	481	250	1.924	24.4
# 8	6	40	897	501	238	2.105	26.7

TABLE 20
Comparable example 2
			Length of
			golf club	Frequency	Frequency		Launching
	Natural	Loft angle θ	shaft	f1	f2	Ratio of	angle
Club #	number X	(degree)	L (mm)	(cpm)	(cpm)	frequencies Z	(degree)
# 3	1	20	962	412	257	1.603	16.1
# 4	2	24	949	422	245	1.722	18.5
# 5	3	28	936	432	252	1.714	20.0
# 6	4	32	923	442	247	1.789	22.1
# 7	5	36	910	452	250	1.808	23.7
# 8	6	40	897	462	227	2.035	27.2

In Table 21, a slope and an intercept in a regression line of ratio of frequencies Z to natural number X, maximum value and minimum value of the difference between the ratio Z of frequencies and the regression line, and a slope and an intercept in a regression line of ratio Z of frequencies to loft angle θ, maximum value and minimum value of the difference between the ratio Z of frequencies and the regression line are shown. Further, in FIG. 35 to FIG. 54, a regression line of ratio Z of frequencies to natural number X of golf club sets in example 1 to 18 and comparative example 1 to 2 is shown. Moreover, in FIG. 55 to FIG. 74, a regression line of ratio Z of frequencies to loft angle θ of golf club sets in example 1 to 18 and comparative example 1 to 2 is shown.

In Table 22, a slope and an intercept in a regression line of ratio of frequencies Z to golf club shaft length L, maximum value and minimum value of the difference between the ratio Z of frequencies and the regression line are shown. Further, in FIG. 75 to FIG. 94, a regression line of ratio Z of frequencies to golf club shaft length L of golf club sets in example 1 to 18 and comparative example 1 to 2 is shown.

	TABLE 21
	Regression line of ratio Z of	Regression line of ratio Z of
	frequencies to natural number X	frequencies to loft angle θ
	Slope	Intercept	Max.	Min.	Slope	Intercept	Max.	Min.
Example 1	−0.277	3.00	0.011	−0.005	−0.069	4.11	0.011	−0.005
Example 2	−0.234	3.03	0.041	−0.036	−0.059	3.97	0.041	−0.036
Example 3	−0.241	2.37	0.017	−0.025	−0.060	3.34	0.017	−0.025
Example 4	−0.245	2.70	0.015	−0.012	−0.061	3.67	0.015	−0.012
Example 5	−0.123	2.09	0.014	−0.012	−0.031	2.58	0.014	−0.012
Example 6	−0.017	1.79	0.037	−0.029	−0.004	1.86	0.037	−0.029
Example 7	−0.029	2.07	0.019	−0.018	−0.007	2.18	0.019	−0.018
Example 8	−0.030	1.41	0.014	−0.009	−0.007	1.53	0.014	−0.009
Example 9	−0.013	1.34	0.013	−0.011	−0.003	1.39	0.013	−0.011
Comparative	−0.144	2.07	0.074	−0.091	−0.036	2.64	0.074	−0.091
example 1
Example	−0.004	1.25	0.014	−0.009	−0.001	1.26	0.014	−0.009
10
Example	0.003	1.34	0.038	−0.027	0.001	1.33	0.038	−0.027
11
Example	0.004	1.78	0.024	−0.015	0.001	1.77	0.024	−0.015
12
Example	0.006	1.91	0.011	−0.014	0.002	1.89	0.011	−0.014
13
Example	0.070	1.43	0.014	−0.008	0.017	1.15	0.014	−0.008
14
Example	0.141	1.20	0.043	−0.020	0.035	0.63	0.043	−0.020
15
Example	0.140	0.94	0.018	−0.025	0.035	0.38	0.018	−0.025
16
Example	0.138	1.42	0.011	−0.014	0.035	0.87	0.011	−0.014
17
Example	0.169	1.08	0.013	−0.011	0.042	0.41	0.013	−0.011
18
Comparative	0.071	1.53	0.078	−0.078	0.018	1.24	0.078	−0.078
example 2

	TABLE 22
	Regression line of
	ratio Z of frequencies
	to length L of golf club shaft
	Slope	Intercept	Max.	Min.
	Example 1	0.0213	−17.75	0.011	−0.005
	Example 2	0.0180	−14.54	0.041	−0.036
	Example 3	0.0185	−15.71	0.017	−0.025
	Example 4	0.0188	−15.65	0.015	−0.012
	Example 5	0.0095	−7.17	0.014	−0.012
	Example 6	0.0013	0.48	0.037	−0.029
	Example 7	0.0023	−0.14	0.019	−0.018
	Example 8	0.0023	−0.84	0.014	−0.009
	Example 9	0.0010	0.36	0.013	−0.011
	Comparative	0.0111	−8.77	0.074	−0.091
	example 1
	Example 10	0.0003	0.95	0.014	−0.009
	Example 11	−0.0002	1.57	0.038	−0.027
	Example 12	−0.0003	2.08	0.024	−0.015
	Example 13	−0.0005	2.39	0.011	−0.014
	Example 14	−0.0053	6.65	0.014	−0.008
	Example 15	−0.0108	11.77	0.043	−0.020
	Example 16	−0.0108	11.44	0.018	−0.025
	Example 17	−0.0106	11.78	0.011	−0.014
	Example 18	−0.0130	13.77	0.013	−0.011
	Comparative	−0.0055	6.87	0.078	−0.078
	example 2

Referring to FIG. 35 to FIG. 94 and Table 21 to 22, it is understood that golf club sets in example 1 to 18 satisfy conditions stipulated in the present invention and golf club sets in comparative example 1 to 2 do not satisfy conditions stipulated in the present invention.

Hitting test using a swing robot of each golf club in the foregoing example 1 to 18 and comparative example 1 to 2 was carried out to measure launching angle of a ball. A swing robot used is Shot Robo 4 manufactured by Miyamae Co. and golf balls used are H/S ball manufactured by Yokohama Rubber Co. Head speed is determined to each club number to hit balls and launching angle just after hitting is measured. Then the average value of ten times hitting is calculated. Head speeds of the swing robot are set as follows: 35.0 m/s for #3, 34.5 m/s for #4, 34.0 m/s for #5, 33.5 m/s for #6, 33.0 m/s for #7, 32.5 m/s for #8. The foregoing launching angles are shown in Table 1 to Table 20 together.

Then regressions line of the launching angles to natural number X in example 1 to 18 and comparative example 1 to 2 are obtained. Then, a range of estimated error of the launching angle to the regression line is obtained, and the results are shown in Table 23. Range of estimated error means the difference between the maximum value and the minimum value among the difference of launching angle and the regression line in each example. Specifically, it is a range between the farthest data from the regression line upward and the farthest data from the regression line downward. Smaller range of the estimated error means more linear correlation between order of the club number (order of size of the loft angle) and height of trajectory of a hit ball.

TABLE 23
	Example 1	Example 2	Example 3	Example 4	Example 5
Range of	0.23	0.55	0.35	0.25	0.16
estimated error
					Comparative
	Example 6	Example 7	Example 8	Example 9	example 1
Range of	0.57	0.36	0.21	0.22	1.45
estimated error
	Example 10	Example 11	Example 12	Example 13	Example 14
Range of	0.25	0.68	0.38	0.19	0.20
estimated error
					Comparative
	Example 15	Example 16	Example 17	Example 18	example 2
Range of	0.61	0.43	0.15	0.20	1.41
estimated error

As shown in Table 23, golf club sets in example 1 to 9 have smaller range of estimated error in comparison with golf club sets in comparative example 1 and it is understood that height of trajectory of a hit ball corresponding to loft angle is obtained through whole set. On the other hand, golf club sets in example 10 to 18 has smaller range of estimated error in comparison with golf club sets in comparative example 2 and it is understood that height of trajectory of a hit ball corresponding to loft angle is obtained through whole set.

In Table 24 to Table 43, club number, natural number X, loft angle θ (degree), golf club shaft length L (mm), frequency f1 (cpm), frequency f2 (cpm), the sum Y (cpm) of frequencies of a golf club set each in example 1 to 18 and comparative example 1 to 2 were shown. Here, frequency f1 is a frequency, the frequency being measured by vibrating a tip portion of a golf club shaft in a state that a rear end portion was fastened for a length of 178 mm from the rear end and a 200 g weight was loaded on the tip portion for a length of 30 mm from the tip end. Frequency f2 is a frequency, the frequency being measured by vibrating the rear end portion in a state that the tip portion was fastened for a length of 178 mm from the tip end and a 200 g weight was loaded on the rear portion for a length of 30 mm from the rear end. The sum Y of frequencies is a sum of frequency f1 and frequency f2.

TABLE 24
Example 1
			Length of
			golf club	Frequency	Frequency	Sum of
	Natural	Loft angle θ	shaft	f1	f2	frequencies	Sum-up
Club #	number X	(degree)	L (mm)	(cpm)	(cpm)	Y (cpm)	marks
# 3	1	20	962	365	280	645	595
# 4	2	24	949	367	285	652	596
# 5	3	28	936	371	282	653	606
# 6	4	32	923	371	285	656	611
# 7	5	36	910	373	283	656	623
# 8	6	40	897	373	282	655	635

TABLE 25
Example 2
			Length of
			golf club	Frequency	Frequency	Sum of
	Natural	Loft angle θ	shaft	f1	f2	frequencies	Sum-up
Club #	number X	(degree)	L (mm)	(cpm)	(cpm)	Y (cpm)	marks
# 3	1	20	962	335	258	593	564
# 4	2	24	949	337	264	601	571
# 5	3	28	936	340	270	610	576
# 6	4	32	923	344	277	621	578
# 7	5	36	910	345	282	627	590
# 8	6	40	897	340	283	623	615

TABLE 26
Example 3
			Length of
			golf club	Frequency	Frequency	Sum of
	Natural	Loft angle θ	shaft	f1	f2	frequencies	Sum-up
Club #	number X	(degree)	L (mm)	(cpm)	(cpm)	Y (cpm)	marks
# 3	1	20	962	376	301	677	633
# 4	2	24	949	384	307	691	632
# 5	3	28	936	386	308	694	649
# 6	4	32	923	387	309	696	667
# 7	5	36	910	394	315	709	665
# 8	6	40	897	393	314	707	691

TABLE 27
Example 4
			Length of
			golf club	Frequency	Frequency	Sum of
	Natural	Loft angle θ	shaft	f1	f2	frequencies	Sum-up
Club #	number X	(degree)	L (mm)	(cpm)	(cpm)	Y (cpm)	marks
# 3	1	20	962	362	265	627	581
# 4	2	24	949	365	271	636	588
# 5	3	28	936	369	275	644	594
# 6	4	32	923	372	278	650	605
# 7	5	36	910	371	281	652	623
# 8	6	40	897	373	284	657	635

TABLE 28
Example 5
			Length of
			golf club	Frequency	Frequency	Sum of
	Natural	Loft angle θ	shaft	f1	f2	frequencies	Sum-up
Club #	number X	(degree)	L (mm)	(cpm)	(cpm)	Y (cpm)	marks
# 3	1	20	962	354	262	616	570
# 4	2	24	949	363	270	633	579
# 5	3	28	936	370	272	642	603
# 6	4	32	923	376	281	657	612
# 7	5	36	910	384	284	668	629
# 8	6	40	897	388	288	676	653

TABLE 29
Example 6
			Length of
			golf club	Frequency	Frequency	Sum of
	Natural	Loft angle θ	shaft	f1	f2	frequencies	Sum-up
Club #	number X	(degree)	L (mm)	(cpm)	(cpm)	Y (cpm)	marks
# 3	1	20	962	370	265	635	602
# 4	2	24	949	385	277	662	609
# 5	3	28	936	395	280	675	641
# 6	4	32	923	409	290	699	651
# 7	5	36	910	421	296	717	672
# 8	6	40	897	423	302	725	712

TABLE 30
Example 7
			Length of
			golf club	Frequency	Frequency	Sum of
	Natural	Loft angle θ	shaft	f1	f2	frequencies	Sum-up
Club #	number X	(degree)	L (mm)	(cpm)	(cpm)	Y (cpm)	marks
# 3	1	20	962	334	238	572	538
# 4	2	24	949	344	250	594	554
# 5	3	28	936	355	261	616	570
# 6	4	32	923	361	271	632	593
# 7	5	36	910	371	281	652	613
# 8	6	40	897	373	289	662	649

TABLE 31
Example 8
			Length
			of golf	Fre-	Fre-	Sum of
	Natural	Loft	club	quency	quency	frequen-
Club	number	angle θ	shaft	f1	f2	cies	Sum-up
#	X	(degree)	L (mm)	(cpm)	(cpm)	Y (cpm)	marks
# 3	1	20	962	383	300	683	629
# 4	2	24	949	395	311	706	647
# 5	3	28	936	403	319	722	671
# 6	4	32	923	411	330	741	693
# 7	5	36	910	420	340	760	713
# 8	6	40	897	424	349	773	744

TABLE 32
Example 9
			Length
			of golf	Fre-	Fre-	Sum of
	Natural	Loft	club	quency	quency	frequen-
Club	number	angle θ	shaft	f1	f2	cies	Sum-up
#	X	(degree)	L (mm)	(cpm)	(cpm)	Y (cpm)	marks
# 3	1	20	962	315	241	556	520
# 4	2	24	949	328	252	580	537
# 5	3	28	936	340	261	601	567
# 6	4	32	923	354	273	627	586
# 7	5	36	910	368	281	649	610
# 8	6	40	897	377	289	666	643

TABLE 33
Comparative example 1
			Length
			of golf	Fre-	Fre-	Sum of
	Natural	Loft	club	quency	quency	frequen-
Club	number	angle θ	shaft	f1	f2	cies	Sum-up
#	X	(degree)	L (mm)	(cpm)	(cpm)	Y (cpm)	marks
# 3	1	20	962	352	273	625	609
# 4	2	24	949	359	293	652	596
# 5	3	28	936	366	293	659	622
# 6	4	32	923	373	303	676	630
# 7	5	36	910	380	297	677	668
# 8	6	40	897	387	298	685	691

TABLE 34
Example 10
			Length
			of golf	Fre-	Fre-	Sum of
	Natural	Loft	club	quency	quency	frequen-
Club	number	angle θ	shaft	f1	f2	cies	Sum-up
#	X	(degree)	L (mm)	(cpm)	(cpm)	Y (cpm)	marks
# 3	1	20	962	297	238	535	497
# 4	2	24	949	314	252	566	518
# 5	3	28	936	328	262	590	550
# 6	4	32	923	343	275	618	576
# 7	5	36	910	357	286	643	609
# 8	6	40	897	367	298	665	642

TABLE 35
Example 11
			Length
			of golf	Fre-	Fre-	Sum of
	Natural	Loft	club	quency	quency	frequen-
Club	number	angle θ	shaft	f1	f2	cies	Sum-up
#	X	(degree)	L (mm)	(cpm)	(cpm)	Y (cpm)	marks
# 3	1	20	962	284	219	503	482
# 4	2	24	949	305	237	542	499
# 5	3	28	936	321	252	573	530
# 6	4	32	923	337	266	603	562
# 7	5	36	910	353	277	630	599
# 8	6	40	897	362	291	653	647

TABLE 36
Example 12
			Length
			of golf	Fre-	Fre-	Sum of
	Natural	Loft	club	quency	quency	frequen-
Club	number	angle θ	shaft	f1	f2	cies	Sum-up
#	X	(degree)	L (mm)	(cpm)	(cpm)	Y (cpm)	marks
# 3	1	20	962	360	266	626	589
# 4	2	24	949	379	285	664	608
# 5	3	28	936	391	299	690	648
# 6	4	32	923	404	315	719	685
# 7	5	36	910	427	327	754	708
# 8	6	40	897	435	341	776	756

TABLE 37
Example 13
			Length
			of golf	Fre-	Fre-	Sum of
	Natural	Loft	club	quency	quency	frequen-
Club	number	angle θ	shaft	f1	f2	cies	Sum-up
#	X	(degree)	L (mm)	(cpm)	(cpm)	Y (cpm)	marks
# 3	1	20	962	377	290	667	617
# 4	2	24	949	396	305	701	643
# 5	3	28	936	414	318	732	675
# 6	4	32	923	428	331	759	716
# 7	5	36	910	449	343	792	743
# 8	6	40	897	462	355	817	784

TABLE 38
Example 14
			Length
			of golf	Fre-	Fre-	Sum of
	Natural	Loft	club	quency	quency	frequen-
Club	number	angle θ	shaft	f1	f2	cies	Sum-up
#	X	(degree)	L (mm)	(cpm)	(cpm)	Y (cpm)	marks
# 3	1	20	962	321	233	554	515
# 4	2	24	949	343	252	595	545
# 5	3	28	936	361	270	631	584
# 6	4	32	923	378	285	663	629
# 7	5	36	910	399	302	701	662
# 8	6	40	897	416	318	734	708

TABLE 39
Example 15
			Length
			of golf	Fre-	Fre-	Sum of
	Natural	Loft	club	quency	quency	frequen-
Club	number	angle θ	shaft	f1	f2	cies	Sum-up
#	X	(degree)	L (mm)	(cpm)	(cpm)	Y (cpm)	marks
# 3	1	20	962	354	278	632	599
# 4	2	24	949	385	298	683	625
# 5	3	28	936	411	315	726	672
# 6	4	32	923	435	331	766	717
# 7	5	36	910	461	349	810	760
# 8	6	40	897	481	361	842	823

TABLE 40
Example 16
			Length
			of golf	Fre-	Fre-	Sum of
	Natural	Loft	club	quency	quency	frequen-
Club	number	angle θ	shaft	f1	f2	cies	Sum-up
#	X	(degree)	L (mm)	(cpm)	(cpm)	Y (cpm)	marks
# 3	1	20	962	274	220	494	467
# 4	2	24	949	300	244	544	499
# 5	3	28	936	320	265	585	544
# 6	4	32	923	343	285	628	586
# 7	5	36	910	360	303	663	641
# 8	6	40	897	381	323	704	687

TABLE 41
Example 17
			Length of
			golf club	Frequency	Frequency	Sum of
	Natural	Loft angle θ	shaft	f1	f2	frequencies	Sum-up
Club #	number X	(degree)	L (mm)	(cpm)	(cpm)	Y (cpm)	marks
# 3	1	20	962	342	262	604	559
# 4	2	24	949	367	284	651	596
# 5	3	28	936	391	300	691	643
# 6	4	32	923	411	320	731	692
# 7	5	36	910	441	336	777	730
# 8	6	40	897	458	356	814	783

TABLE 42
Example 18
			Length of
			golf club	Frequency	Frequency	Sum of
	Natural	Loft angle θ	shaft	f1	f2	frequencies	Sum-up
Club #	number X	(degree)	L (mm)	(cpm)	(cpm)	Y (cpm)	marks
# 3	1	20	962	383	262	645	598
# 4	2	24	949	409	286	695	640
# 5	3	28	936	433	307	740	688
# 6	4	32	923	457	331	788	735
# 7	5	36	910	479	355	834	783
# 8	6	40	897	501	374	875	840

TABLE 43
Comparative example 2
			Length of
			golf club	Frequency	Frequency	Sum of
	Natural	Loft angle θ	shaft	f1	f2	frequencies	Sum-up
Club #	number X	(degree)	L (mm)	(cpm)	(cpm)	Y (cpm)	marks
# 3	1	20	962	296	222	518	510
# 4	2	24	949	317	240	557	543
# 5	3	28	936	338	267	605	560
# 6	4	32	923	359	278	637	605
# 7	5	36	910	380	297	677	634
# 8	6	40	897	401	297	698	704

In FIG. 95 to FIG. 114, relations between natural number X and the sum Y of frequencies of a golf club set each in example 1 to 18 and comparative example 1 to 2 are shown. Moreover, in FIG. 115 to FIG. 134, relations between loft angle θ and the sum Y of frequencies of a golf club set each in example 1 to 18 and comparative example 1 to 2 are shown. In FIG. 95 to FIG. 134, two parallel straight lines putting all plotted points therebetween are written together.

In Table 44, a slope and an intercept in a regression line of the sum of frequencies Y to natural number X, maximum value and minimum value of the difference between the sum Y of frequencies and the regression line, and a slope and an intercept in a regression line of the sum Y of frequencies to loft angle θ, maximum value and minimum value of the difference between the sum Y of frequencies and the regression line are shown. Further in FIG. 135 to FIG. 154, a regression line of the sum Y of frequencies to natural number X of a golf club set each in example 1 to 18 and comparative example 1 to 2 is shown. Further, in FIG. 155 to FIG. 174, a regression line of the sum Y of frequencies to loft angle θ of a golf club set each in example 1 to 18 and comparative example 1 to 2 is shown.

In Table 45, a slope and an intercept in a regression line of the sum Y of frequencies to golf club shaft length L, maximum value and minimum value of the difference between the sum Y of frequencies and the regression line are shown. Further, in FIG. 175 to FIG. 194, a regression line of the sum Y of frequencies to golf club shaft length L of a golf club set each in example 1 to 18 and comparative example 1 to 2 is shown.

	TABLE 44
	Regression line of
	sum Y of frequencies	Regression line of sum Y of
	to natural number X	frequencies to loft angle θ
		Inter-				Inter-
	Slope	cept	Max.	Min.	Slope	cept	Max.	Min.
Example 1	1.86	646	2.2	−3.2	0.46	639	2.2	−3.2
Example 2	6.83	589	5.1	−6.6	1.71	561	5.1	−6.6
Example 3	5.89	675	4.5	−4.0	1.47	652	4.5	−4.0
Example 4	5.83	624	2.8	−2.8	1.46	601	2.8	−2.8
Example 5	12.00	607	2.3	−2.7	3.00	559	2.3	−2.7
Example 6	18.26	622	4.4	−6.1	4.56	549	4.4	−6.1
Example 7	18.29	557	3.8	−5.0	4.57	484	3.8	−5.0
Example 8	18.03	668	2.2	−2.9	4.51	596	2.2	−2.9
Example 9	22.37	535	2.6	−3.1	5.59	445	2.6	−3.1
Comparative	11.20	623	8.1	−9.3	2.80	578	8.1	−9.3
example 1
Example	25.97	512	2.2	−2.9	6.49	408	2.2	−2.9
10
Example	29.83	480	4.1	−6.4	7.46	360	4.1	−6.4
11
Example	29.97	600	4.2	−3.9	7.49	480	4.2	−3.9
12
Example	30.00	640	2.3	−2.7	7.50	520	2.3	−2.7
13
Example	35.71	521	2.5	−3.0	8.93	378	2.5	−3.0
14
Example	42.03	596	3.8	−6.2	10.51	428	3.8	−6.2
15
Example	41.43	458	4.3	−5.4	10.36	292	4.3	−5.4
16
Example	41.94	565	2.8	−2.5	10.49	397	2.8	−2.5
17
Example	46.14	601	2.1	−3.2	11.54	417	2.1	−3.2
18
Comparative	36.91	486	8.1	−9.6	9.23	338	8.1	−9.6
example 2

	TABLE 45
	Regression line of
	sum Y of frequencies
	to length L of golf club shaft
	Slope	Intercept	Max.	Min.
	Example 1	−0.14	786	2.2	−3.2
	Example 2	−0.53	1101	5.1	−6.6
	Example 3	−0.45	1116	4.5	−4.0
	Example 4	−0.45	1061	2.8	−2.8
	Example 5	−0.92	1507	2.3	−2.7
	Example 6	−1.40	1991	4.4	−6.1
	Example 7	−1.41	1929	3.8	−5.0
	Example 8	−1.39	2020	2.2	−2.9
	Example 9	−1.72	2213	2.6	−3.1
	Comparative	−0.86	1463	8.1	−9.3
	example 1
	Example	−2.00	2460	2.2	−2.9
	10
	Example	−2.29	2717	4.1	−6.4
	11
	Example	−2.31	2848	4.2	−3.9
	12
	Example	−2.31	2890	2.3	−2.7
	13
	Example	−2.75	3200	2.5	−3.0
	14
	Example	−3.23	3748	3.8	−6.2
	15
	Example	−3.19	3565	4.3	−5.4
	16
	Example	−3.23	3710	2.8	−2.5
	17
	Example	−3.55	4062	2.1	−3.2
	18
	Comparative	−2.84	3255	8.1	−9.6
	example 2

Referring to FIG. 95 to FIG. 194 and Table 44, 45, it is understood that golf club sets in example 1 to 18 satisfy conditions stipulated in the present invention and golf club sets in comparative example 1 to 2 do not satisfy conditions stipulated in the present invention.

Hitting tests of each golf club in the foregoing example 1 to 18 and comparative example 1 to 2 are carried out. In the hitting tests, a golfer hits 5 balls with each golf club and evaluated feeling of flexibility of golf club shafts. Evaluation marks are as follows: 1 is soft, 2 is slightly soft, 3 is normal, 4 is slightly stiff, 5 is stiff. A golfer hits 5 balls with a golf club but indicates one evaluation mark. Specifically, flexibility feeling of a golf club is evaluated as the result of hitting 5 balls with the golf club. Evaluation mentioned above is performed by 200 golfers.

With regard to the foregoing evaluation marks, marks by 200 people are summed up for each golf club to obtain sum-up marks. It may be said that full score is 5 (maximum score)×200 (number of golfers)=1000. This sum-up marks are written in Table 24 to Table 43 together. This numerical value of sum-up marks is based on marks evaluated on flexibility of golf club shafts by 200 golfers as mentioned above, and it can be said that it indicates flexibility of golf club shaft quantitatively.

Then a regression line of sum-up marks to natural number X of a golf club set each in example 1 to 18 and comparative example 1 to 2 is obtained, and range of estimated error of sum-up marks to the regression line is obtained. The results are shown in Table 46. The range of estimated error means the difference between maximum value and minimum value among difference between sum-up marks and a regression line in each example. Specifically, it is a range between the farthest data from the regression line upward and the farthest data from the regression line downward. Smaller range of the estimated error means more linear correlation between order of the club number (order of size of the loft angle) and flexibility of golf club shafts.

TABLE 46
	Example 1	Example 2	Example 3	Example 4	Example 5
Range of	8.5	19.1	14.5	9.1	8.4
estimated error
					Comparative
	Example 6	Example 7	Example 8	Example 9	example 1
Range of	18.6	14.4	8.3	8.6	33.3
estimated error
	Example 10	Example 11	Example 12	Example 13	Example 14
Range of	8.8	19.2	14.9	9.2	8.9
estimated error
					Comparative
	Example 15	Example 16	Example 17	Example 18	example 2
Range of	18.9	15.4	8.5	8.8	33.6
estimated error

As shown in Table 46, range of estimated error of golf club sets in example 1 to 9 is smaller than that of golf club sets in comparative example 1, and it is understood that flexibility of golf club shafts are well controlled through a whole set. On the other hand, range of estimated error of golf club sets in example 10 to 18 is smaller than that of golf club sets in comparative example 2, and it is understood that flexibility of golf club shafts are well controlled through a whole set.

As mentioned above, preferred embodiments in the present invention were described in detail, and it should be understood that various changes, substitutions and replacements to those can be performed as far as those do not digressed from spirit and scope in the present invention stipulated in the attached claim.

Claims

1. A golf club shaft set comprising a plurality of golf club shafts to constitute a golf club set, wherein, in at least three golf club shafts among the plurality of golf club shafts, a sum of a first frequency, the first frequency being measured by vibrating a tip portion of each of the golf club shafts in a state that a rear end portion of the golf club shaft is fastened, and a second frequency, the second frequency being measured by vibrating the rear end portion of the golf club shaft in a state that the tip portion of the golf club shaft is fastened, is determined in relation with order of length of the golf club shaft, and wherein the sum of frequencies is varied corresponding to order of length of the golf club shaft substantially linearly.

2. A golf club shaft set comprising a plurality of golf club shafts to constitute a golf club set, wherein the plurality of golf club shafts include a group of at least three golf club shafts, and, when length of the golf club shafts in the group are denoted by L (mm) and a sum of a first frequency, the first frequency being measured by vibrating a tip portion of each of the golf club shafts in a state that a rear end portion of the golf club shaft is fastened for a length of 178 mm from the rear end and a 200 g weight is loaded on the tip portion for a length of 30 mm from the tip end, and a second frequency, the second frequency being measured by vibrating the rear end portion of the golf club shaft in a state that the tip portion of the golf club shaft is fastened for a length of 178 mm from the tip end and a 200 g weight is loaded on the rear end portion for a length of 30 mm from the rear end, is denoted by y (cpm), the sum y of frequencies is determined so that an estimated error to a regression line is 8 (cpm) or less, when a distribution of the sum y of frequencies to the length L of the golf club shaft in all of the golf club shafts in the group is fitted on the regression line, and wherein a slope of the regression line of the sum y of frequencies to the length L is −1.85 or less.

3. The golf club shaft set according to claim 2, wherein the group of the golf club shafts comprises golf club shafts to be assembled to golf clubs having loft angles in a range of 16 degree or more and 41 degree or less.

4. The golf club shaft set according to claim 2, wherein, when a ratio of frequencies calculated from a frequency as a numerator, the frequency being measured in the state that the rear end portion of the golf club shaft is fastened, and a frequency as a denominator, the frequency being measured in the state that the tip portion of the golf club shaft is fastened, is denoted by Z, the ratio Z of frequencies is determined so that an estimated error to a regression line is 0.15 or less, when a distribution of the ratio Z of frequencies to the length L in all of the golf club shafts in the group is fitted on the regression line.

5. The golf club shaft set according to any one of claims 1, 2, 3, and 4, wherein the golf club shaft is made of fiber reinforced plastics.